Parton Densities and Fragmentation Functions from Polarized Lambda Production in Semi-Inclu
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stable diffusion 摄影术语稳定扩散(stable diffusion)是摄影术语中的一个概念,指的是使用特定的技术手段在摄影作品中创造出一种模糊、柔和、温暖的效果,给人一种梦幻、浪漫、温馨的感觉。
稳定扩散常常被用于人像摄影和风光摄影中,以营造出一种柔和、温暖的氛围,使照片更加有韵味、有吸引力。
稳定扩散可以通过使用滤镜、调整设备设置、后期处理等多种方式来实现。
下面将详细介绍几种常见的稳定扩散实现方法。
一、使用滤镜:1. 扩散镜(Soft Focus Filter)是一种非常常见的稳定扩散滤镜,其主要作用是增加整个图像的柔和程度。
扩散镜利用镜片表面的纹理,模糊图像的细节,同时给予整个画面一个温暖而柔和的效果。
不同的扩散镜有不同的纹理和颗粒大小,可以根据需要选择。
2. 透镜镀层滤镜(Lens Coating Filter)是另一种常见的稳定扩散滤镜,它可以改变物体的反射和折射,使光线分散并产生一个柔和的效果。
透镜镀层滤镜常常用于拍摄阳光照射的场景,可以创造出太阳光穿过树叶间隙的效果。
3. 灰度滤镜(Neutral Density Filter)是一种常用的稳定扩散滤镜,它用于平衡不同场景中的曝光差异。
灰度滤镜可以使高亮区域变得柔和,避免过曝的现象。
通过选择不同的灰度滤镜,可以调整图像的扩散程度和整体效果。
二、调整设备设置:1. 光圈设置:选择较大的光圈值(如f/1.8、f/2.8等)可以减小景深,使前景和背景更模糊,从而创造出一种柔和的效果。
2. 快门速度:使用较长的快门速度(如1/30秒、1/60秒等)可以使相机在拍摄过程中有微小的晃动,从而产生一种轻微的模糊效果,增加稳定扩散的效果。
3. ISO设置:选择较低的ISO值(如ISO 100、ISO 200等)可以降低图像噪点,使图像更加柔和。
在充足的光线条件下使用低ISO值可以得到更好的效果。
三、后期处理:1. 软化滤镜:在后期处理中,可以使用软化滤镜或模糊工具来增加图像的扩散效果。
密度函数理论和杜比宁方程可以用来研究活性炭纤维在多段充填过程中的吸附行为。
密度函数理论是一种分子统计力学理论,它建立在分子统计学和热力学的基础上,用来研究一种系统中分子的分布。
杜比宁方程是一种描述分子吸附行为的方程,它可以用来计算吸附层的厚度、吸附速率和吸附能量等参数。
在研究活性炭纤维多段充填过程中,可以使用密度函数理论和杜比宁方程来研究纤维表面的分子结构和吸附行为。
通过分析密度函数和杜比宁方程的解,可以得出纤维表面的分子结构以及纤维吸附的分子的种类、数量和能量。
这些信息有助于更好地理解活性炭纤维的多段充填机理。
在研究活性炭纤维的多段充填机理时,还可以使用其他理论和方法来帮助我们更好地了解这一过程。
例如,可以使用扫描电子显微镜(SEM)和透射电子显微镜(TEM)等技术来观察纤维表面的形貌和结构。
可以使用X射线衍射(XRD)和傅里叶变换红外光谱(FTIR)等技术来确定纤维表面的化学成分和结构。
还可以使用氮气吸附(BET)和旋转氧吸附(BJH)等技术来测量纤维表面的比表面积和孔结构。
通过综合运用密度函数理论、杜比宁方程和其他理论和方法,可以更全面地了解活性炭纤维的多段充填机理,从而更好地控制和优化多段充填的过程。
在研究活性炭纤维多段充填机理时,还可以使用温度敏感性测试方法来研究充填过程中纤维表面的动力学性质。
例如,可以使用动态氧吸附(DAC)或旋转杆氧吸附(ROTA)等技术来测量温度对纤维表面吸附性能的影响。
通过对比不同温度下纤维表面的吸附性能,可以更好地了解充填过程中纤维表面的动力学性质。
此外,还可以使用分子动力学模拟方法来研究纤维表面的吸附行为。
例如,可以使用拉曼光谱或红外光谱等技术来测量纤维表面的分子吸附构型。
然后,使用分子动力学模拟方法来模拟不同分子吸附构型下的纤维表面的动力学性质,帮助我们更好地了解活性炭纤维的多段充填机理。
多肽固相合成步骤英文描述多肽固相合成是一种合成肽链的方法,它涉及到多个步骤。
以下是多肽固相合成的步骤和英文描述:1. 准备载体:选择适当的树脂,如弱碱性丙烯酰胺树脂(Acrylamide resin)。
Prepare resin: select an appropriate resin, such as weakly basic acrylamide resin.2. 载体预处理:将树脂进行预处理,如使用二氯甲烷和二甲基甲酰胺进行交替洗涤,实现树脂表面的清洁和活化。
Pre-treatment of the resin: pre-treat the resin, such as alternating washing with dichloromethane and dimethylformamide to achieve a clean and activated resin surface.3. 防止侧反应:在肽链合成过程中,需要采取措施防止侧反应的发生,例如使用保护基。
Prevent side reactions: measures need to be taken to prevent side reactions during peptide synthesis, such as using protective groups.4. 合成肽链:通过加入氨基酸单元和活化剂,将肽链逐步合成。
Synthesize the peptide chain: synthesize the peptide chain step by step by adding amino acid units and activators.5. 洗脱肽链:用酸性溶液或氢氟酸将肽链从树脂上洗脱。
Elute the peptide chain: elute the peptide chain from the resin using an acidic solution or hydrogen fluoride.6. 去保护基:使用适当的溶液去除保护基。
【高分子专业英语翻译】第五课乳液聚合大部分的乳液聚合都是由自由基引发的并且表现出其他自由基体系的很多特点,最主要的反应机理的不同源自小体积元中自由基增长的场所不同。
乳液聚合不仅允许在高反应速率下获得较高分子量,这在本体聚合中是无法实现或效率低下的,,同时还有其他重要的实用优点。
水吸收了大部分聚合热且有利于反应控制,产物在低粘度体系中获得,容易处理,可直接使用或是在凝聚,水洗,干燥之后很快转化成固体聚合物。
在共聚中,尽管共聚原理适用于乳液体系,单体在水相中溶解能力的不同也可能导致其与本体聚合行为不同,从而有重要的实际意义。
乳液聚合的变化很大,从包含单一单体,乳化剂,水和单一引发剂的简单体系到这些包含有2,3个单体,一次或分批添加,,混合乳化剂和助稳定剂以及包括链转移剂的复合引发体系。
单体和水相的比例允许变化范围很大,但是在技术做法上通常限制在30/70到60/40。
单体和水相比更高时则达到了直接聚合允许的极限,只有通过分批添加单体方法来排除聚合产生的大量的热。
更复杂的是随着胶体数的增加粘度也大大增加,尤其是当水溶性的单体和聚合物易容时,反应结束胶乳浓度降低。
这一阶段常常伴随着通过聚集作用或是在热力学不稳定时凝结作用而使胶粒尺寸增大。
第十课高分子的构型和构象本课中我们将使用根据经典有机化学术语而来的构型和构象这两个词。
构型异构是由于分子中存在一个或多个不对称中心,以最简单的C原子为例,每一碳原子的绝对构型为R型和S型,当存在双键时会有顺式和反式几何异构。
以合成聚合物为例,构型异构的典型问题和R.S型不对称碳原子在主链上的排布有关。
这些不对称碳原子要么来自不对称单体,如环氧丙烷,要么来自对称单体,如乙烯单体,,这些物质的聚合,在每个单体单元中形成至少一个不对称碳原子。
大分子中的构型异构源于侧链上存在不对称的碳原子,例如不对称乙烯单体的聚合,也是可能的,现今已经被广泛研究。
和经典有机化学术语一致,构象,旋转体,旋转异构体,构象异构体,指的是由于分子单键的内旋转而形成的空间排布的不同。
斯仑贝谢所有测井曲线英文名称解释OCEAN DRILLING PROGRAMACRONYMS USED FOR WIRELINE SCHLUMBERGER TOOLS ACT Aluminum Clay ToolAMS Auxiliary Measurement SondeAPS Accelerator Porosity SondeARI Azimuthal Resistivity ImagerASI Array Sonic ImagerBGKT Vertical Seismic Profile ToolBHC Borehole Compensated Sonic ToolBHTV Borehole TeleviewerCBL Casing Bond LogCNT Compensated Neutron ToolDIT Dual Induction ToolDLL Dual LaterologDSI Dipole Sonic ImagerFMS Formation MicroScannerGHMT Geologic High Resolution Magnetic ToolGPIT General Purpose Inclinometer ToolGR Natural Gamma RayGST Induced Gamma Ray Spectrometry ToolHLDS Hostile Environment Lithodensity SondeHLDT Hostile Environment Lithodensity ToolHNGS Hostile Environment Gamma Ray SondeLDT Lithodensity ToolLSS Long Spacing Sonic ToolMCD Mechanical Caliper DeviceNGT Natural Gamma Ray Spectrometry ToolNMRT Nuclear Resonance Magnetic ToolQSST Inline Checkshot ToolSDT Digital Sonic ToolSGT Scintillation Gamma Ray ToolSUMT Susceptibility Magnetic ToolUBI Ultrasonic Borehole ImagerVSI Vertical Seismic ImagerWST Well Seismic ToolWST-3 3-Components Well Seismic ToolOCEAN DRILLING PROGRAMACRONYMS USED FOR LWD SCHLUMBERGER TOOLSADN Azimuthal Density-NeutronCDN Compensated Density-NeutronCDR Compensated Dual ResistivityISONIC Ideal Sonic-While-DrillingNMR Nuclear Magnetic ResonanceRAB Resistivity-at-the-BitOCEAN DRILLING PROGRAMACRONYMS USED FOR NON-SCHLUMBERGER SPECIALTY TOOLSMCS Multichannel Sonic ToolMGT Multisensor Gamma ToolSST Shear Sonic ToolTAP Temperature-Acceleration-Pressure ToolTLT Temperature Logging ToolOCEAN DRILLING PROGRAMACRONYMS AND UNITS USED FOR WIRELINE SCHLUMBERGER LOGSAFEC APS Far Detector Counts (cps)ANEC APS Near Detector Counts (cps)AX Acceleration X Axis (ft/s2)AY Acceleration Y Axis (ft/s2)AZ Acceleration Z Axis (ft/s2)AZIM Constant Azimuth for Deviation Correction (deg)APLC APS Near/Array Limestone Porosity Corrected (%)C1 FMS Caliper 1 (in)C2 FMS Caliper 2 (in)CALI Caliper (in)CFEC Corrected Far Epithermal Counts (cps)CFTC Corrected Far Thermal Counts (cps)CGR Computed (Th+K) Gamma Ray (API units)CHR2 Peak Coherence, Receiver Array, Upper DipoleCHRP Compressional Peak Coherence, Receiver Array, P&SCHRS Shear Peak Coherence, Receiver Array, P&SCHTP Compressional Peak Coherence, Transmitter Array, P&SCHTS Shear Peak Coherence, Transmitter Array, P&SCNEC Corrected Near Epithermal Counts (cps)CNTC Corrected Near Thermal Counts (cps)CS Cable Speed (m/hr)CVEL Compressional Velocity (km/s)DATN Discriminated Attenuation (db/m)DBI Discriminated Bond IndexDEVI Hole Deviation (degrees)DF Drilling Force (lbf)DIFF Difference Between MEAN and MEDIAN in Delta-Time Proc. (microsec/ft) DRH HLDS Bulk Density Correction (g/cm3)DRHO Bulk Density Correction (g/cm3)DT Short Spacing Delta-Time (10'-8' spacing; microsec/ft)DT1 Delta-Time Shear, Lower Dipole (microsec/ft)DT2 Delta-Time Shear, Upper Dipole (microsec/ft)DT4P Delta- Time Compressional, P&S (microsec/ft)DT4S Delta- Time Shear, P&S (microsec/ft))DT1R Delta- Time Shear, Receiver Array, Lower Dipole (microsec/ft)DT2R Delta- Time Shear, Receiver Array, Upper Dipole (microsec/ft)DT1T Delta-Time Shear, Transmitter Array, Lower Dipole (microsec/ft)DT2T Delta-Time Shear, Transmitter Array, Upper Dipole (microsec/ft)DTCO Delta- Time Compressional (microsec/ft)DTL Long Spacing Delta-Time (12'-10' spacing; microsec/ft)DTLF Long Spacing Delta-Time (12'-10' spacing; microsec/ft)DTLN Short Spacing Delta-Time (10'-8' spacing; microsec/ftDTRP Delta-Time Compressional, Receiver Array, P&S (microsec/ft)DTRS Delta-Time Shear, Receiver Array, P&S (microsec/ft)DTSM Delta-Time Shear (microsec/ft)DTST Delta-Time Stoneley (microsec/ft)DTTP Delta-Time Compressional, Transmitter Array, P&S (microsec/ft)DTTS Delta-Time Shear, Transmitter Array, P&S (microsec/ft)ECGR Environmentally Corrected Gamma Ray (API units)EHGR Environmentally Corrected High Resolution Gamma Ray (API units) ENPH Epithermal Neutron Porosity (%)ENRA Epithermal Neutron RatioETIM Elapsed Time (sec)FINC Magnetic Field Inclination (degrees)FNOR Magnetic Field Total Moment (oersted)FX Magnetic Field on X Axis (oersted)FY Magnetic Field on Y Axis (oersted)FZ Magnetic Field on Z Axis (oersted)GR Natural Gamma Ray (API units)HALC High Res. Near/Array Limestone Porosity Corrected (%)HAZI Hole Azimuth (degrees)HBDC High Res. Bulk Density Correction (g/cm3)HBHK HNGS Borehole Potassium (%)HCFT High Resolution Corrected Far Thermal Counts (cps)HCGR HNGS Computed Gamma Ray (API units)HCNT High Resolution Corrected Near Thermal Counts (cps)HDEB High Res. Enhanced Bulk Density (g/cm3)HDRH High Resolution Density Correction (g/cm3)HFEC High Res. Far Detector Counts (cps)HFK HNGS Formation Potassium (%)HFLC High Res. Near/Far Limestone Porosity Corrected (%)HEGR Environmentally Corrected High Resolution Natural Gamma Ray (API units) HGR High Resolution Natural Gamma Ray (API units)HLCA High Res. Caliper (inHLEF High Res. Long-spaced Photoelectric Effect (barns/e-)HNEC High Res. Near Detector Counts (cps)HNPO High Resolution Enhanced Thermal Nutron Porosity (%)HNRH High Resolution Bulk Density (g/cm3)HPEF High Resolution Photoelectric Effect (barns/e-)HRHO High Resolution Bulk Density (g/cm3)HROM High Res. Corrected Bulk Density (g/cm3)HSGR HNGS Standard (total) Gamma Ray (API units)HSIG High Res. Formation Capture Cross Section (capture units) HSTO High Res. Computed Standoff (in)HTHO HNGS Thorium (ppm)HTNP High Resolution Thermal Neutron Porosity (%)HURA HNGS Uranium (ppm)IDPH Phasor Deep Induction (ohmm)IIR Iron Indicator Ratio [CFE/(CCA+CSI)]ILD Deep Resistivity (ohmm)ILM Medium Resistivity (ohmm)IMPH Phasor Medium Induction (ohmm)ITT Integrated Transit Time (s)LCAL HLDS Caliper (in)LIR Lithology Indicator Ratio [CSI/(CCA+CSI)]LLD Laterolog Deep (ohmm)LLS Laterolog Shallow (ohmm)LTT1 Transit Time (10'; microsec)LTT2 Transit Time (8'; microsec)LTT3 Transit Time (12'; microsec)LTT4 Transit Time (10'; microsec)MAGB Earth's Magnetic Field (nTes)MAGC Earth Conductivity (ppm)MAGS Magnetic Susceptibility (ppm)MEDIAN Median Delta-T Recomputed (microsec/ft)MEAN Mean Delta-T Recomputed (microsec/ft)NATN Near Pseudo-Attenuation (db/m)NMST Magnetometer Temperature (degC)NMSV Magnetometer Signal Level (V)NPHI Neutron Porosity (%)NRHB LDS Bulk Density (g/cm3)P1AZ Pad 1 Azimuth (degrees)PEF Photoelectric Effect (barns/e-)PEFL LDS Long-spaced Photoelectric Effect (barns/e-)PIR Porosity Indicator Ratio [CHY/(CCA+CSI)]POTA Potassium (%)RB Pad 1 Relative Bearing (degrees)RHL LDS Long-spaced Bulk Density (g/cm3)RHOB Bulk Density (g/cm3)RHOM HLDS Corrected Bulk Density (g/cm3)RMGS Low Resolution Susceptibility (ppm)SFLU Spherically Focused Log (ohmm)SGR Total Gamma Ray (API units)SIGF APS Formation Capture Cross Section (capture units)SP Spontaneous Potential (mV)STOF APS Computed Standoff (in)SURT Receiver Coil Temperature (degC)SVEL Shear Velocity (km/s)SXRT NMRS differential Temperature (degC)TENS Tension (lb)THOR Thorium (ppm)TNRA Thermal Neutron RatioTT1 Transit Time (10' spacing; microsec)TT2 Transit Time (8' spacing; microsec)TT3 Transit Time (12' spacing; microsec)TT4 Transit Time (10' spacing; microsec)URAN Uranium (ppm)V4P Compressional Velocity, from DT4P (P&S; km/s)V4S Shear Velocity, from DT4S (P&S; km/s)VELP Compressional Velocity (processed from waveforms; km/s)VELS Shear Velocity (processed from waveforms; km/s)VP1 Compressional Velocity, from DT, DTLN, or MEAN (km/s)VP2 Compressional Velocity, from DTL, DTLF, or MEDIAN (km/s)VCO Compressional Velocity, from DTCO (km/s)VS Shear Velocity, from DTSM (km/s)VST Stonely Velocity, from DTST km/s)VS1 Shear Velocity, from DT1 (Lower Dipole; km/s)VS2 Shear Velocity, from DT2 (Upper Dipole; km/s)VRP Compressional Velocity, from DTRP (Receiver Array, P&S; km/s) VRS Shear Velocity, from DTRS (Receiver Array, P&S; km/s)VS1R Shear Velocity, from DT1R (Receiver Array, Lower Dipole; km/s) VS2R Shear Velocity, from DT2R (Receiver Array, Upper Dipole; km/s) VS1T Shear Velocity, from DT1T (Transmitter Array, Lower Dipole; km/s) VS2T Shear Velocity, from DT2T (Transmitter Array, Upper Dipole; km/s) VTP Compressional Velocity, from DTTP (Transmitter Array, P&S; km/s) VTS Shear Velocity, from DTTS (Transmitter Array, P&S; km/s)#POINTS Number of Transmitter-Receiver Pairs Used in Sonic Processing W1NG NGT Window 1 counts (cps)W2NG NGT Window 2 counts (cps)W3NG NGT Window 3 counts (cps)W4NG NGT Window 4 counts (cps)W5NG NGT Window 5 counts (cps)OCEAN DRILLING PROGRAMACRONYMS AND UNITS USED FOR LWD SCHLUMBERGER LOGSAT1F Attenuation Resistivity (1 ft resolution; ohmm)AT3F Attenuation Resistivity (3 ft resolution; ohmm)AT4F Attenuation Resistivity (4 ft resolution; ohmm)AT5F Attenuation Resistivity (5 ft resolution; ohmm)ATR Attenuation Resistivity (deep; ohmm)BFV Bound Fluid Volume (%)B1TM RAB Shallow Resistivity Time after Bit (s)B2TM RAB Medium Resistivity Time after Bit (s)B3TM RAB Deep Resistivity Time after Bit (s)BDAV Deep Resistivity Average (ohmm)BMAV Medium Resistivity Average (ohmm)BSAV Shallow Resistivity Average (ohmm)CGR Computed (Th+K) Gamma Ray (API units)DCAL Differential Caliper (in)DROR Correction for CDN rotational density (g/cm3).DRRT Correction for ADN rotational density (g/cm3).DTAB AND or CDN Density Time after Bit (hr)FFV Free Fluid Volume (%)GR Gamma Ray (API Units)GR7 Sum Gamma Ray Windows GRW7+GRW8+GRW9-Equivalent to Wireline NGT window 5 (cps) GRW3 Gamma Ray Window 3 counts (cps)-Equivalent to Wireline NGT window 1GRW4 Gamma Ray Window 4 counts (cps)-Equivalent to Wireline NGT window 2GRW5 Gamma Ray Window 5 counts (cps)-Equivalent to Wireline NGT window 3GRW6 Gamma Ray Window 6 counts (cps)-Equivalent to Wireline NGT window 4GRW7 Gamma Ray Window 7 counts (cps)GRW8 Gamma Ray Window 8 counts (cps)GRW9 Gamma Ray Window 9 counts (cps)GTIM CDR Gamma Ray Time after Bit (s)GRTK RAB Gamma Ray Time after Bit (s)HEF1 Far He Bank 1 counts (cps)HEF2 Far He Bank 2 counts (cps)HEF3 Far He Bank 3 counts (cps)HEF4 Far He Bank 4 counts (cps)HEN1 Near He Bank 1 counts (cps)HEN2 Near He Bank 2 counts (cps)HEN3 Near He Bank 3 counts (cps)HEN4 Near He Bank 4 counts (cps)MRP Magnetic Resonance PorosityNTAB ADN or CDN Neutron Time after Bit (hr)PEF Photoelectric Effect (barns/e-)POTA Potassium (%) ROPE Rate of Penetration (ft/hr)PS1F Phase Shift Resistivity (1 ft resolution; ohmm)PS2F Phase Shift Resistivity (2 ft resolution; ohmm)PS3F Phase Shift Resistivity (3 ft resolution; ohmm)PS5F Phase Shift Resistivity (5 ft resolution; ohmm)PSR Phase Shift Resistivity (shallow; ohmm)RBIT Bit Resistivity (ohmm)RBTM RAB Resistivity Time After Bit (s)RING Ring Resistivity (ohmm)ROMT Max. Density Total (g/cm3) from rotational processing ROP Rate of Penetration (m/hr)ROP1 Rate of Penetration, average over last 1 ft (m/hr).ROP5 Rate of Penetration, average over last 5 ft (m/hr)ROPE Rate of Penetration, averaged over last 5 ft (ft/hr)RPM RAB Tool Rotation Speed (rpm)RTIM CDR or RAB Resistivity Time after Bit (hr)SGR Total Gamma Ray (API units)T2 T2 Distribution (%)T2LM T2 Logarithmic Mean (ms)THOR Thorium (ppm)TNPH Thermal Neutron Porosity (%)TNRA Thermal RatioURAN Uranium (ppm)OCEAN DRILLING PROGRAMADDITIONAL ACRONYMS AND UNITS(PROCESSED LOGS FROM GEOCHEMICAL TOOL STRING)AL2O3 Computed Al2O3 (dry weight %)AL2O3MIN Computed Al2O3 Standard Deviation (dry weight %) AL2O3MAX Computed Al2O3 Standard Deviation (dry weight %) CAO Computed CaO (dry weight %)CAOMIN Computed CaO Standard Deviation (dry weight %) CAOMAX Computed CaO Standard Deviation (dry weight %) CACO3 Computed CaCO3 (dry weight %)CACO3MIN Computed CaCO3 Standard Deviation (dry weight %) CACO3MAX Computed CaCO3 Standard Deviation (dry weight %) CCA Calcium Yield (decimal fraction)CCHL Chlorine Yield (decimal fraction)CFE Iron Yield (decimal fraction)CGD Gadolinium Yield (decimal fraction)CHY Hydrogen Yield (decimal fraction)CK Potassium Yield (decimal fraction)CSI Silicon Yield (decimal fraction)CSIG Capture Cross Section (capture units)CSUL Sulfur Yield (decimal fraction)CTB Background Yield (decimal fraction)CTI Titanium Yield (decimal fraction)FACT Quality Control CurveFEO Computed FeO (dry weight %)FEOMIN Computed FeO Standard Deviation (dry weight %) FEOMAX Computed FeO Standard Deviation (dry weight %) FEO* Computed FeO* (dry weight %)FEO*MIN Computed FeO* Standard Deviation (dry weight %) FEO*MAX Computed FeO* Standard Deviation (dry weight %) FE2O3 Computed Fe2O3 (dry weight %)FE2O3MIN Computed Fe2O3 Standard Deviation (dry weight %) FE2O3MAX Computed Fe2O3 Standard Deviation (dry weight %) GD Computed Gadolinium (dry weight %)GDMIN Computed Gadolinium Standard Deviation (dry weight %) GDMAX Computed Gadolinium Standard Deviation (dry weight %) K2O Computed K2O (dry weight %)K2OMIN Computed K2O Standard Deviation (dry weight %)K2OMAX Computed K2O Standard Deviation (dry weight %) MGO Computed MgO (dry weight %)MGOMIN Computed MgO Standard Deviation (dry weight %) MGOMAX Computed MgO Standard Deviation (dry weight %)S Computed Sulfur (dry weight %)SMIN Computed Sulfur Standard Deviation (dry weight %) SMAX Computed Sulfur Standard Deviation (dry weight %)SIO2 Computed SiO2 (dry weight %)SIO2MIN Computed SiO2 Standard Deviation (dry weight %) SIO2MAX Computed SiO2 Standard Deviation (dry weight %) THORMIN Computed Thorium Standard Deviation (ppm) THORMAX Computed Thorium Standard Deviation (ppm)TIO2 Computed TiO2 (dry weight %)TIO2MIN Computed TiO2 Standard Deviation (dry weight %) TIO2MAX Computed TiO2 Standard Deviation (dry weight %) URANMIN Computed Uranium Standard Deviation (ppm) URANMAX Computed Uranium Standard Deviation (ppm) VARCA Variable CaCO3/CaO calcium carbonate/oxide factor。
APT Attached Proton Test 质子连接实验ASIS Aromatic Solvent Induced Shift 芳香溶剂诱导位移BBDR Broad Band Double Resonance 宽带双共振BIRD Bilinear Rotation Decoupling 双线性旋转去偶(脉冲)COLOC Correlated Spectroscopy for Long Range Coupling 远程偶合相关谱COSY ( Homonuclear chemical shift ) COrrelation SpectroscopY (同核化学位移)相关谱CP Cross Polarization 交叉极化CP/MAS Cross Polarization / Magic Angle Spinning 交叉极化魔角自旋CSA Chemical Shift Anisotropy 化学位移各向异性CSCM Chemical Shift Correlation Map 化学位移相关图CW continuous wave 连续波DD Dipole-Dipole 偶极-偶极DECSY Double-quantum Echo Correlated Spectroscopy 双量子回波相关谱DEPT Distortionless Enhancement by Polarization Transfer 无畸变极化转移增强2DFTS two Dimensional FT Spectroscopy 二维傅立叶变换谱DNMR Dynamic NMR 动态NMRDNP Dynamic Nuclear Polarization 动态核极化DQ(C) Double Quantum (Coherence) 双量子(相干)DQD Digital Quadrature Detection 数字正交检测DQF Double Quantum Filter 双量子滤波DQF-COSY Double Quantum Filtered COSY 双量子滤波COSY DRDS Double Resonance Difference Spectroscopy 双共振差谱EXSY Exchange Spectroscopy 交换谱FFT Fast Fourier Transformation 快速傅立叶变换FID Free Induction Decay 自由诱导衰减H,C-COSY 1H,13C chemical-shift COrrelation SpectroscopY 1H,13C 化学位移相关谱H,X-COSY 1H,X-nucleus chemical-shift COrrelation SpectroscopY1H,X-核化学位移相关谱HETCOR Heteronuclear Correlation Spectroscopy 异核相关谱HMBC Heteronuclear Multiple-Bond Correlation 异核多键相关HMQC Heteronuclear Multiple Quantum Coherence异核多量子相干HOESY Heteronuclear Overhauser Effect Spectroscopy 异核Overhause效应谱HOHAHA Homonuclear Hartmann-Hahn spectroscopy 同核Hartmann-Hahn谱HR High Resolution 高分辨HSQCHeteronuclear Single Quantum Coherence 异核单量子相干INADEQUATE Incredible Natural Abundance Double Quantum Transfer Experiment 稀核双量子转移实验(简称双量子实验,或双量子谱)INDOR Internuclear Double Resonance 核间双共振INEPT Insensitive Nuclei Enhanced by Polarization 非灵敏核极化转移增强INVERSE H,X correlation via 1H detection 检测1H的H,X核相关IR Inversion-Recovery 反(翻)转回复JRES J-resolved spectroscopy J-分解谱LIS Lanthanide (chemical shift reagent ) Induced Shift 镧系(化学位移试剂)诱导位移LSR Lanthanide Shift Reagent 镧系位移试剂MAS Magic-Angle Spinning 魔角自旋MQ(C) Multiple-Quantum ( Coherence ) 多量子(相干)MQF Multiple-Quantum Filter 多量子滤波MQMAS Multiple-Quantum Magic-Angle Spinning 多量子魔角自旋MQS Multi Quantum Spectroscopy 多量子谱NMR Nuclear Magnetic Resonance 核磁共振NOE Nuclear Overhauser Effect 核Overhauser效应(NOE)NOESY Nuclear Overhauser Effect Spectroscopy 二维NOE谱NQR Nuclear Quadrupole Resonance 核四极共振PFG Pulsed Gradient Field 脉冲梯度场PGSE Pulsed Gradient Spin Echo 脉冲梯度自旋回波PRFT Partially Relaxed Fourier Transform 部分弛豫傅立叶变换PSD Phase-sensitive Detection 相敏检测PW Pulse Width 脉宽RCT Relayed Coherence Transfer 接力相干转移RECSY Multistep Relayed Coherence Spectroscopy 多步接力相干谱REDOR Rotational Echo Double Resonance 旋转回波双共振RELAY Relayed Correlation Spectroscopy 接力相关谱RF Radio Frequency 射频ROESY Rotating Frame Overhauser Effect Spectroscopy 旋转坐标系NOE谱ROTO ROESY-TOCSY Relay ROESY-TOCSY 接力谱SC Scalar Coupling 标量偶合SDDS Spin Decoupling Difference Spectroscopy 自旋去偶差谱SE Spin Echo 自旋回波SECSY Spin-Echo Correlated Spectroscopy自旋回波相关谱SEDOR Spin Echo Double Resonance 自旋回波双共振SEFT Spin-Echo Fourier Transform Spectroscopy (with J modulation)(J-调制)自旋回波傅立叶变换谱SELINCOR Selective Inverse Correlation 选择性反相关SELINQUATE Selective INADEQUATE 选择性双量子(实验)SFORD Single Frequency Off-Resonance Decoupling 单频偏共振去偶SNR or S/N Signal-to-noise Ratio 信 / 燥比SQF Single-Quantum Filter 单量子滤波SR Saturation-Recovery 饱和恢复TCF Time Correlation Function 时间相关涵数TOCSY Total Correlation Spectroscopy 全(总)相关谱TORO TOCSY-ROESY Relay TOCSY-ROESY接力TQF Triple-Quantum Filter 三量子滤波WALTZ-16 A broadband decoupling sequence 宽带去偶序列WATERGATE Water suppression pulse sequence 水峰压制脉冲序列WEFT Water Eliminated Fourier Transform 水峰消除傅立叶变换ZQ(C) Zero-Quantum (Coherence) 零量子相干ZQF Zero-Quantum Filter 零量子滤波T1 Longitudinal (spin-lattice) relaxation time for MZ 纵向(自旋-晶格)弛豫时间T2 Transverse (spin-spin) relaxation time for Mxy 横向(自旋-自旋)弛豫时间tm mixing time 混合时间τc rotational correlation time 旋转相关时间。
Surface Science Reports63(2008)487–513Contents lists available at ScienceDirectSurface Science Reports journal homepage:/locate/surfrepHigh-throughput heterogeneous catalysisDavid Farrusseng∗UniversitéLyon1,CNRS,UMR5256,IRCELYON,Institut de recherches sur la catalyse et l’environnement de Lyon,2avenue Albert Einstein,F-69626Villeurbanne,Francea r t i c l e i n f o Article history:Accepted16September2008 editor:W.H.Weinberg Keywords:CatalysisCombinatorial chemistryHigh-throughputKinetic modelingQSAR a b s t r a c tThis comprehensive review of the literature(over250references)deals with high-throughput experimentation in heterogeneous catalysis.Approaches to library design for catalyst discovery and optimization are described and discussed.Special focus is placed on advanced methods for knowledge discovery such as high-throughput kinetic modeling and QSAR.An inventory of successful case studies in catalysis is reported.Finally,recent developments in relevant electronic data and knowledge management are described.©2008Published by Elsevier B.V.Contents1.Introduction (488)2.Overview (488)3.Approaches to HT library design (489)3.1.The split&pool method (489)3.2.The hierarchical approach (490)3.3.Design of experiments(DoE)methodology(See also Figs.4and5) (492)3.4.Evolutionary algorithms (493)3.5.Evolutionary optimization using data mining tools (495)3.6.Summary (496)4.HT kinetic modeling (496)4.1.Reasons for conducting HT kinetic modeling (496)4.2.Technologies for HT kinetic modeling (497)4.3.Methodologies of HT kinetic modeling (497)4.4.Spatially-and time-resolved methods (499)5.The QSAR approach to catalysis (500)5.1.Generalities (500)5.2.Homogeneous catalysis and the QSAR approach (500)5.2.1.The QSAR concept (500)5.2.2.In silico generation of a virtual catalyst library (501)5.2.3.Choice and calculation of descriptors (501)5.2.4.QSAR modeling (501)5.3.Heterogeneous catalysis and the QSAR approach (502)5.4.HT physicochemical characterization for property quantification (502)5.5.Catalyst profiling using HT kinetic modeling of model reactions (503)5.6.Virtual screening through computational chemistry (504)Abbreviations:AniML,Analytical Information Markup Language;ANN,Artificial Neural Networks;ANOVA,Analysis Of Variance;DFT,Density Functional Theory;DoE, Design of Experiments;ee,enantioselectivity;FPA,Focalplane;FTIR,Fourier Transform Infrared;GA,Genetic Algorithm;GDC,Guided Data Capture;HT,High-throughput; HTE,High-throughput Experimentation;IT,Information Technology;KFE,Kinetic Fitting Engine;LRIS,Laboratory Research Informatic System;PCA,Principal Component Analysis;QM,Quantum Mechanics;QSAR,Quantitative Structure–Activity Relationship;QSPR,Quantitative Structure–Property Relationship;SCR,Selective Catalytic Reduction;SMEs,Small and Medium Enterprises;TPD,Temperature-programmed Desorption;TOF,Turnover Frequency;TON,Turnover Number;WGS,Water-gas Shift; WHSV,Weight Hourly Space Velocity;XML,Extensible Markup Language;XRD,X-ray Diffraction;XRF,X-ray Fluorescence.∗Tel.:+33472445365;fax:+33472445399.E-mail address:david.farrusseng@ircelyon.univ-lyon1.fr.0167-5729/$–see front matter©2008Published by Elsevier B.V.doi:10.1016/j.surfrep.2008.09.001488 D.Farrusseng/Surface Science Reports63(2008)487–5136.Discovery of catalytic materials by HT (504)6.1.Electrocatalysts for fuel cells (504)6.2.Selective hydrocarbon oxidation (504)6.3.Hydrogen production and purification (505)6.4.Automotive and refinery applications (505)6.5.Other applications (505)6.6.HT experimentation for zeolite synthesis and discoveries (505)7.Electronic infrastructure (506)7.1.Why automate data treatment? (506)7.2.Electronic open architecture for tool integration (506)7.2.1.HTE AG electronic platform (506)7.2.2.The NIST vision (506)7.2.3.Academic laboratories (507)7.2.4.Workflow-based electronic infrastructure for streamline data processing and knowledge management (507)7.2.5.Data normalization and e-standards in chemistry (509)8.Conclusions (509)Acknowledgements (510)References (510)1.IntroductionOver80%of commercial chemical processes involve the use of catalysis,with products as varied as chemicals,oil products, fertilizers,plastics,drugs and pharmaceuticals being made through catalytic steps.Catalysis is probably the most important means of producing modern chemicals;Europe’s chemical industry,for example,accounts for e1.5trillion,or14%,of this continent’s e10.5 trillion GDP(Gross Domestic Product).The likelihood of innovation in this field decreases,however, as catalytic chemical processes become increasingly mature. When new active solids are developed empirically,by trial-and-error processes employed on a few selected samples,the whole procedure is highly speculative and leads to a very slow rate of discovery for the industry in question.This research strategy based on exhaustive studies and complete understanding is also very time-consuming.Therefore,new research strategies have to be developed in order to produce breakthroughs and revitalize the field of chemical research.The high-throughput(HT)approach is a pragmatic alternative. It relies on the fast and systematic screening of libraries of diverse samples.This methodology is not new,since its origins can be found at different periods of the last century.One of the most striking examples is the discovery of the first ammonia synthesis catalyst by Mittasch et al.at BASF in1909followed by a‘‘systematic investigation of the periodic table’’with about 20,000experiments[1].This approach also appealed to K.Ziegler, who in the1950s applied it to the discovery of polymerization catalysts.The pragmatic approach of that time aimed at exploring and covering the periodic table;no references to HT screening or sample libraries could yet be made.We can trace the modern HT approach back to the pioneering work of Hanak in the1970s. He prepared and applied what we now call composition-spread or gradient libraries for research and development purposes at the RCA company laboratories.His work led to the successful entry of several new products onto the market[2].His vision of the experimental approach brought materials screening into the modern age:‘‘...the present approach to the search for new materials suffers from a chronic ailment,that of handling one sample at a time in the processes of synthesis,analysis and testing of properties.It is an expensive and time-consuming approach,which prevents highly-trained personnel from taking full advantage of its talents and keeps the tempo of discovery of new materials at a low level’’[3].The combinatorial principles employed in drug development were first applied to materials research in the early1990s by physi-cists and materials scientists at the Lawrence Berkeley National Laboratory of UC Berkeley.In fact,combinatorial materials sci-ence was recognized as a bona fide discipline only a few years later,following this team’s famous search for superconductors us-ing a materials library[4–7].By1997,the recently-formed Symyx Technologies had documented the state of the art of combinato-rial chemistry by publishing a library of over25,000distinct com-pounds[8].From2000onward,HT technology has been developed for and applied to an ever-increasing variety of materials,including electronic and magnetic materials,polymer-based materials,opti-cal materials,biomaterials,paints,drug formulations,detergents, cosmetics and glues,with the number of related publications and patents exploding accordingly.Today,HT experimentation has matured and is almost regarded as commonplace,its use in the development of new materials sometimes being omitted from a publication’s title or abstract,or even from the publication rge chemical companies (such as BASF,BP,Bayer,Degussa,DOW,DuPont,Exxon,GE, and UOP LLC)now generally have their own HT tools or labs. Meanwhile,smaller companies specialized in HT experimentation (such as Avantium,Bosch Lab Systems,hte AG,Symyx Technologies and Torial)have been founded,often enjoying spectacular growth in the space of the last ten years.Specialized companies such as these have succeeded thanks to their development of cutting-edge technologies,including hardware and software as well as their tight integration,that provide an impressive degree of throughput and productivity(number of samples screened per day and further decision making).In such a context of technological sophistication and high productivity,most academic groups have found themselves unable to compete in the race that is materials screening.Instead,public research centers can play a major role in HT by conducting fundamental research on domains as varied as synthetic methods,analytical tools,parallel in situ characterization,data mining and decision making processes and, finally–the focus of this review–screening strategies and methods.This review deals mainly with HT experimentation for hetero-geneous catalysis and also briefly discusses homogeneous cataly-sis.For other disciplines of materials science,the reader can refer to various reviews[9–19],books[20,21]and special issues[22–30]. An excellent summary of the state of the art for materials science has recently been published elsewhere[31].2.OverviewSince HT screening is a methodological approach,this review is divided into sections describing particular HT screening strategies and their associated strengths,issues,solutions,and case studies.What are the general issues affecting HT experimentation?D.Farrusseng/Surface Science Reports63(2008)487–513489Thanks to the modern screening techniques used in HT methods,dozens or even hundreds of experiments involving many variables can be performed at once.The inevitable combinatorial explosion that results leads to two urgent,fundamental questions relating to experimental design:which experiments are the most relevant to carry out,and what is the most efficient screening strategy?Data analysis is the next issue to come up after the experimental design is chosen.It is hardly possible for humans to fully evaluate results and statistical trends emanating from data sets involving more than four variables and20experiments.The issue of decision making takes on particular importance in such a scenario.In order to understand a catalytic process,one must be aware of the most relevant variables and combinations of variables affecting it.Catalysis,and chemistry in general, are matters of synergy and typically involve highly non-linear behaviors[32],as in metal–ligand or metal–support interactions for homogeneous and heterogeneous catalysis,respectively.Once the exploratory data analysis reveals whether it is possible to highlight positive interactions,and whether one can identify and quantify trends between variables and catalytic performances,a decision must be made—what is the most relevant experimental set to perform next?Computational methods employing mathematics,statistics and artificial intelligence are required for scientists to deal adequately with these three key issues influencing HT experimentation: experimental design,data analysis,and decision making.For over15years,these issues have been addressed in the field of drug discovery,leading to the emergence of a brand new domain of science with its own specialized journals.Section5deals with the application of such screening strategies and their related tools to HT catalyst design,as well as recent developments in the application of quantitative structure–activity relationship(QSAR) to homogeneous and heterogeneous catalysis,with an emphasis on the differences between organic and inorganic compounds in terms of descriptors.Kinetic modeling,on the other hand,reflects the scientist’s insight into the chemical kinetics and,therefore,provides useful information about catalyst behavior.It relates feedstock and operating conditions to reaction rates and corresponding effluent composition,thereby quantifying catalytic performances.Recent kinetic models also contain so-called catalyst descriptors,which specifically account for catalyst properties such as the number of sites and the reactant chemisorption enthalpy.Section4addresses the concepts,recent advances and limitations of kinetic modeling in HT experimentation.An appropriate electronic infrastructure for HT screening is absolutely necessary in order to prevent bottlenecks.Manual entry and cutting-and-pasting of data are to be minimized in order to limit the impact of erroneous entries and slowed-down experiments.Section7addresses these issues,with examples describing and illustrating current technology.Publications,handbooks and other documents available over the Internet,whether free of charge or at a fee,have rendered accessible a great deal of data that could possibly generate knowledge and assist in the decision-making process.That said,the direct capture of data is usually prevented due to the heterogeneity of data,as well as to a lack of standards regarding not just data format but also document format(*.pdf or*.html).The emergence of new technologies,concerted worldwide organizations for electronic standards and new business models appears to be changing this situation.This review does not deal only with catalyst design but also with the optimization of the process conditions due to the strong interplay between catalyst,reactor design and experimental testing conditions.Sections 3.1–3.3address the issues of HT strategies and library design,while Section4explores the benefits of using kinetic and transient approaches for catalyst design.3.Approaches to HT library designThe objectives of a targeted study,such as the discovery of entirely new compounds by exploring large search spaces or the fine optimization of a known catalyst[33,34],have a strong impact on the selection of an appropriate screening strategy and the associated information technology tools.Equipment constraints,synthesis feasibility and screening performances are also important factors to panies or HT departments have developed tailor-made solutions and entire workflows.The issues of HT infrastructure and tool integration as described in[35] will not be discussed here.This section describes the various screening strategies developed in industry and academia,in order from the simplest to the most complex strategies and algorithms, and to some extent from the most massive to the most qualitative screening.3.1.The split&pool methodIn the context of a primary screening aiming to identify hits in a very large search space,the split&pool approach, derived from pharmaceutical methodology,is especially well-suited.It is generally employed in ambitious catalyst discovery programs or when little is known about the target reaction and the class of materials to be studied.Even with a limited number of variables,several hundred samples can easily be obtained thanks to the combinatorial explosion.High analytical speed and overall throughput usually take precedence over the quality or density of information obtained.The split&pool approach enables the generation of every possible combination in a search space.While the generation methodology is quite simple,the major issue,due to its complexity, is the recognition of a molecule in a mixture.For this purpose, many different techniques have been developed to tag molecules, but such techniques cannot be directly applied to inorganic solids. Detailed below are two different tagging strategies,developed by UOP LLC and hte AG,that do allow tagging in the context of inorganic solids.In both strategies,one finds a massive parallel arrangement of micro-reaction chambers containing individual beads,each bead representing one catalyst as a member of a library of solid catalysts.This provides the advantages of easy catalyst handling(unlike the case of powders),very small quantities of metal precursors(typically100µg per catalyst)and a synthesis protocol that can be scaled up.At UOP,catalysts are tagged by using spatially addressable arrays such as microtiter plates(i.e.,96-well plates)[36].Each well contains a single catalyst bead which is indexed by four coordinates,namely the well-plate identity,row and column numbers and split and synthesis step.The combinatorial synthesis consists of a multi-step metal salt impregnation with intermediate drying.Once the metal salt solution is adsorbed onto the beads and dried,rows of beads from a given plate are transferred using a row-sorter to a set of receiving well plates.The sorting algorithm can be set in such a way that the sequence of row-and column-shuffling steps monitors the compositional redundancy of the resulting split–pool library.This process makes it possible for classic,inexpensive laboratory equipment to perform the synthesis of compositionally diverse libraries.The hte AG company has developed fast parallel post-analysis, an alternative to2D addressable layout tagging[37–40].The‘‘split’’step of the split&pool synthesis consists of dividing a few thousand beads into a number of equal portions placed on porcelain dishes. The beads,which are roughly1mm in diameter and are typical catalytic supports,such as alumina or titania,are impregnated with different metallic salt solutions varying by concentration or by metal nature,and then calcined.The beads are then recombined490 D.Farrusseng /Surface Science Reports 63(2008)487–513Fig.1.Split and pool synthesis (a),micro-bead reactor (b)after [39].Table 1Binary composition at the first screening.For each binary system,8different compositions are synthesized using a linear gradientapproach.(‘‘pooled’’)together and are well-mixed via shaking.Typically,the whole process is repeated several times.For example,for five different metal precursors at four different concentrations,the beads are split five times into four different containers (Fig.1).The total number of possible combinations from a mathematical perspective is 45=1024.That said,because the synthesis protocol cannot guarantee that each bead will follow a different path (making the preparation of some identical catalysts possible),it is recommended to start with a greater number of beads,with a ratio of 1.2–1.5with respect to the total theoretical number of combinations.At hte AG,up to 625beads can be tested individually by fast sequential testing methods in a specially-designed array of micro-reactors.The ‘‘hits’’identified are then post-analyzed by micro-X-ray fluorescence (or micro-XRF).In only a few minutes,commercial equipment can quantify the composition of an array of 100samples.The knowledge of the presence or absence of elements and of the range of concentration makes it possible to trace the synthesis path history for the beads.3.2.The hierarchical approachSome erroneous measurements inevitably occur during the primary screening due to the extreme miniaturization and the great number of experiments.Inactive catalysts can appear as ‘‘hits’’(false positives)and active catalysts that should be selected are missed (false negatives).In primary screening,false negatives (which would be missed forever)are far more problematic than are false positives (which would be discarded anyway following the secondary screening).With this fact in mind,Symyx has developed screening strategies to reduce the likelihood of false negatives.Over a two-week period in Symyx laboratories,a hierarchical gradient approach was used with MoVNb patented catalysts for ethane partial oxidation to acetic acid [41].This process led to the discovery of new dopants and to the successful rediscovery of existing catalysts.The primary screening is targeted to identify the best ternary combinations of redox metals from V,Mo,Cr,Mn,Fe,Co,Ni,Cu,Ag,Re,Sn,Sb,Ti and Bi.At the outset,30redox binary systems were investigated,with eight distinct samples synthesizedfor each binary system using a gradient approach consisting of a linear evolution of the composition (Table 1).Of the 30redox binaries (8-point gradients),MoV is by far the most active redox binary,while other active binaries are CrV,MnV,MnCr,CeV,CoCr,CoV,VTi and MoTi.Next,an additional element X was investigated within the MoV system,with X =Mg ,Cr ,Li ,Nb ,Mn ,Co ,Cu ,Fe ,Ni ,Zn ,Zr ,Sb ,Ag ,In or Ce,plus three proprietary dopants.For each ternary,12–15distinct compositions were screened.It was found that Nb,Ni,Sb,and Ce,as well as the three proprietary dopants,result in higher acetic acid productivity.Finally,among the 18ternary MoVX systems,eight of the most promising were tested again with 28different compositions per ternary system.In agreement with the literature,the MoVNb system was identified as very active,while several other metal dopants also produced hits.In summary,as the screening proceeds,the number of com-ponents in the catalytic system increases,formulation complexity increases and higher degrees of interactions are sought in a step-wise manner.The gradient library design approach also permits the efficient management of false negatives and false positives.The testing of similar compositions greatly reduces the risk of missing a hit,while allowing for the easy identification of false positives which afterward are not subjected to further screening.Symyx has demonstrated the value of this screening strategy for various types of catalysis,allowing the determination of the best formulations already reported in the literature and the discovery of new sys-tems [42].For example,the efficiency of Ni–Co–Nb and Ni–Ta–Nb oxide catalysts has successfully been proven for the ethane ox-idative dehydrogenation process at low temperatures [43],while supported-CoCr mixed oxide catalyst systems are proposed for VOC removal [44].Academic laboratories have also applied the gradient strategy.In a primary screening for the partial oxidation of isobutane [45–48],nine elements (V,Fe,Mo,Cr,Ta,Nb,Mn,Sb and Bi)were selected for an initial library design due to the promising partial oxidation properties reported in the literature for the associated oxides.As an alternative to a hierarchical approach,a single library was composed of the nine single oxides (AO x ),D.Farrusseng/Surface Science Reports63(2008)487–513491Fig.2.Emissivity-corrected IR-thermographic images of catalyst library during methanation of CO2at200◦C from[59].of double mixed oxides(A a B b O x)and of ternary mixed oxides (A a B b C c O x).The double mixed oxides consisted of all possible pairs with molar composition(0:1),(0.25:0.75),(0.5:0.5),(0.75:0.25) and(1:0)starting from the nine elements.The ternary mixed oxides consisted of combinations of three elements,always with a(0.33:0.33:0.33)molar composition.Most of the best dehydrogenation catalysts turned out to be Mn and Cr mixed oxides.In accordance with these results,four focused ternary systems–MoVSbO x,MoVFeO x,MoVBiO x and VBiSbO x–were studied in more detail using a dense grinding of the search space. The three elements were allowed to vary between0and100mol% in steps of10mol%,which led to the preparation of66samples per ternary.Other ternaries were investigated elsewhere[49].According to the authors,such composition-spread libraries should allow the identification of any existing local maxima. The best-performing mixed oxides among MoVSbO x,MoVFeO x, MoVBiO x and VBiSbO x were scaled up and tested in a secondary screening.The result was that the optimized composition, Mo10V10Sb80O x,surpassed the best reference catalyst in the literature.Several screening devices have been developed for the mapping of composition-spread libraries.Infrared(IR)thermography is an appropriate choice for the identification of active components in primary screening because,in principle,thousands of samples can be analyzed at the same time[11,50–61].This system records the temperature change arising from the exothermicity or endothermicity of the reaction(Fig.2).In principle,theselectivity Fig.3.Cross-section of the assembled reactor(left)and magnification of reaction chambers(right)from[70].Fig.4.Experimental planning for catalyst design(left).Headers correspond to the element names on the right;M,O,D and S stand for noble Metal,metal Oxides,Dopants and Supports,respectively.Main effects of catalyst compositions on the CO conversion(right),in the absence of H2(a)and in the presence of H2(b).492 D.Farrusseng /Surface Science Reports 63(2008)487–513Fig.5.Blocking structure of 19×19metal binary library (left).Results of 19×19metal binary study (right);synergy was calculated as the difference between the observed TON for the combination minus the sum of the TONs for the individual metals [77].can be measured using an IR focal plane detector [62–65].Other alternatives were developed to overcome selectivity measurement issues such as the use of mass spectrometry (MS)equipped with capillary sampling as shown in [66–70,44,49,71–73].Devices combining IR thermography for rapid hit identification and MS analysis have also been developed [40,74].See also Fig.3.3.3.Design of experiments (DoE)methodology (See also Figs.4and 5)DoE methodology,which involves the simultaneous modifi-cation of variables (usually called factors)and the avoidance of redundant experiments,is widely used in the domain of process engineering.Even though their algorithms are based on simple linear regression,DoE tools can be applied to different objectives that are of particular value in HT experimentation.By means of homogeneous sampling,DoE can be used to efficiently explore a large search space defined by many discrete variables,while guar-anteeing maximal efficiency in terms of the information gleaned from experiments.DoE methodology,when used for screening purposes,quantifies the effect of each individual variable on the targeted properties and identifies the variables relevant to further rounds of screening.On the other hand,when one seeks informa-tion regarding catalytic mechanisms or metal or metal–support synergisms,special DoE design also allows the quantification of in-teractions between variables.Finally,when all relevant variables have been identified,DoE planning is very efficient for the fine op-timization of both catalyst synthesis and process conditions.In this case,the most robust surface responses are generated as empirical models while minimizing the number of experiments.Recent pub-lications illustrate the versatility and power of DoE applied to HT catalyst experimentation.At TU Delft,three sequential DoEs were carried out to find a new one-pot route for the catalytic hydrogenation of acylated cyanohydrins to N -acyl β-amino alcohols [75].Both catalyst formulations and process conditions were varied within the first screening,as shown in Table 2.A selection of 24reactions out of the 320total possible combinations was performed through the use of a D-optimal algorithm.This design is appropriate in view of discarding irrelevant variables for further rounds of optimization.New insights derived from the first design allowed a second one to be carried out using the parameters indicated in Table 3.Variables showing very little impact were discarded.On the other hand,since the nature of the support appeared to bear major importance,a new support,silica,was introduced in the search space.The now considerably reduced parameter space rendered feasible a full-factorial design (i.e.,36combinations),providing accurate information on the main effects of the parameters and especially on the interactions between the parameters.In suchTable 2Definition of the parameter search space for the first screening round.Table 3Definition of the parameter search space for the second screening round.designs,about half the possible number of reactions are typically performed.Finally,a third design was performed in conventional reactors,taking into account other variables such as pressure and temperature.A strategy of sequential hierarchical designs is believed to be better than a single large one,because the information obtained from one design is used to improve the next.If one large DoE design had been chosen,many unnecessary reactions would have been performed.Preliminary designs (typically fewer than 25%of the possible reactions)are sufficient to allow differentiation between significant and insignificant parameters,and are therefore well-suited to reduce the search space in the early stages of the research effort.The search for selective CO oxidation catalysts for H 2purifica-tion applications has also been a context for using a very similar hi-erarchical strategy using a D-optimal design algorithm for primary screening [76].An a priori selection of elements and of combinato-rial rules for mixing them and generating multi-component cata-lysts was performed according to literature data and pre-existing knowledge.Four groups of elements were considered:noble met-als (Pt,Pd,Ru,Rh and Au),oxides (transition metal oxides of Cr,Co,Mn,La,Sm and Mo),dopants (alkali or earth alkali Li,Cs and Ca)and supports (Al 2O 3,CeO 2,ZrO 2,ZnO and C).One of the a priori rules established was that all catalysts were to be composed of one sup-port and two noble metals and,optionally,of one transition metal and one dopant.The weight percentages of noble metal,as well as transition metal and dopant (when present),were fixed at 0.5%,20%and 1%,respectively.The choice to employ two distinct noble metals per catalyst was based on the assumption that alloys may。
·研究论著·急性间质性肺炎一例并文献复习巴俊慧石云锋冯定云吴本权【摘要】目的探讨急性间质性肺炎(AIP)的病因、诊断与治疗,提高对该病的认识水平。
方法对1例一氧化碳中毒后迟发性脑病患者发生AIP的临床资料进行回顾性分析,并以“急性间质性肺炎”或“acute interstitial pneumonia”为检索词在PubMed、中国期刊全文数据库(CNKI)、万方数据知识服务平台和维普中文科技期刊数据库检索,收集并分析检索到的有详细症状、诊断、治疗、转归的病例资料。
结果该例为21岁的一氧化碳中毒后迟发性脑病女性患者,因呼吸衰竭转入内科ICU,经抗感染治疗无效,病理活组织检查(活检)诊断为AIP,予肾上腺皮质激素(激素)、环磷酰胺、机械通气等治疗后好转出院。
检索文献后,排除已知AIP诱发因素的病例,157例有详细症状、诊断、治疗、转归的病例资料,其中72例经病理活检确诊。
AIP患者的主要临床表现为咳嗽(141例,89.8%)、呼吸困难(130例,82.8%)、发热(79例,50.3%),主要影像学表现为磨玻璃样变(119例,75.8%)、肺实变(37例,23.6%)、弥漫性渗出影(33例,21.0%);主要病理活检表现为Ⅱ型肺泡上皮增生(24例,33.3%)、肺泡纤维化(22例,30.6%)、肺泡间隔增厚(20例,27.8%);使用大剂量激素治疗44例(28.0%),联合免疫抑制剂治疗12例(7.6%),行机械通气100例(63.7%);体外膜肺氧合(4例,2.5%);共57例(36.3%)患者好转出院,100例(63.7%)患者死亡。
结论AIP是一种病因未明、起病急骤、以呼吸衰竭为主的间质性肺炎,目前无疗效确切的治疗方法,早期激素治疗可能有效,临床预后差。
【关键词】急性间质性肺炎;肺损伤;高压氧Acute interstitial pneumonia:one case report and literature review Ba Junhui,Shi Yunfeng,Feng Din⁃gyun,Wu Benquan.Medical Intensive Care Unit,the Third Affiliated Hospital of Sun Yat⁃sen University,Guangzhou510630,ChinaCorresponding author,Wu Benquan,E⁃mail:【Abstract】Objective To analyze the pathogenesis,diagnosis and treatment of acute interstitial pneu⁃monia(AIP)and deepen the understanding of AIP.Methods Clinical data of one patient with delayed en⁃cephalopathy suffering from AIP after carbonic oxide poisoning were retrospectively analyzed.A comprehensive literature search was performed in PubMed,China Journal Full⁃text Database(CNKI),Wanfang Data and Chongqing Vip database using the keywords of"acute interstitial pneumonia"in both English and Chinese.De⁃tailed clinical data including symptoms,diagnosis,treatment and outcomes of patients with AIP were collectedand analyzed.Results The21⁃year⁃old female patient diagnosed with delayed encephalopathy was transferred tothe MICU due to respiratory failure after carbonic oxide poisoning.She was not effectively treated after antibiotic therapy.She was diagnosed with AIP by pathological tissue examination(lung biopsy),Then,the patient wastreated with steroid,cyclophosphamide,and mechanical ventilation.She was recovered and discharged.After excluding patients whose inducing factors of AIP have been identified,detailed symptoms,diagnosis,treat⁃ment and outcomes were collected from157AIP patients,and72cases of them were confirmed by pathological biopsy.The clinical manifestations of AIP patients mainly included cough(n=141,89.8%),dyspnea(n=130,82.8%)and fever(n=79,50.3%).The main imaging findings consisted of ground glass changes(n=119,75.8%),pulmonary consolidation(n=37,23.6%)and diffuse exudative lesions(n=33,21.0%).DOI:10.3969/j.issn.0253⁃9802.2018.12.010基金项目:广东省科技计划项目(2017A020215177)作者单位:510630,广州,中山大学附属第三医院内科ICU(巴俊慧,石云锋,吴本权),呼吸内科(冯定云)通讯作者,吴本权,E⁃The dominant pathological findings were typeⅡalveolar epithelial hyperplasia(n=24,33.3%),alveolar fi⁃brosis(n=22,30.6%)and thickening of alveolar septum(n=20,27.8%).Forty⁃four cases(28.0%)were treated with high⁃dose hormone therapy,12(7.6%)were supplemented with immunosuppressive agents,100(63.7%)received mechanical ventilation and4cases were treated with ECMO(2.5%).A total of57 patients(36.3%)were recovered and discharged,whereas100patients(63.7%)died.Conclusions AIP is a category of interstitial lung disease with unknown pathogenesis,urgent onset which rapidly develops in⁃to respiratory failure.At present,there is no exactly effective treatment.Early steroid therapy may be beneficial to patients,but the clinical prognosis of AIP patients is rather poor.【Key words】Acute interstitial pneumonia;Lung injury;Hyperbaric oxygen急性间质性肺炎(AIP)是临床中罕见的、发展迅速的暴发性肺损伤,患者可急进性出现通气功能障碍和呼吸衰竭,病死率可达50%以上。
P element P因⼦[果蝇的可动遗传因⼦,会造成杂种不育,可⽤作外源基因的载体]P nucleotide P核苷酸[见于免疫球蛋⽩及T细胞受体等基因,为重排中根据模板信息所插⼊]pacemaker 起搏点,起搏器pacemaker enzyme 定步酶pachynema 粗线期packaging 包装packaging ratio 包装率[⼀条染⾊单体基本纤维的全长与DNA双螺旋的全长之⽐,反映DNA分⼦的凝聚状态] packed 填充的packed cellvolume 收集细胞体积[⽤以表⽰培养物的相对增长率]paddle blender 浆式捣碎器[利⽤往复运动的浆叶捣碎密封塑料袋中的材料]paedogenetic parthenogenesis 幼体孤雌⽣殖paired sib method 同胞对照法pairing 配对palindrome 回⽂序列,回⽂结构palindromic sequence 回⽂序列palisade tissue 栅栏组织palytoxin 岩沙海葵毒素pancreas 胰腺pancreastatin 胰抑制素[可抑制胰岛素分泌]pancreatic 胰的pancreatin 胰酶制剂pancreozymin 促伊妹⼉素panmixis 随机交配panning 淘选panning technique 淘选技术[如通过亲和层析纯化细胞]panose 潘糖panoxadiol ⼈参⼆醇panoxatriol ⼈参三醇pantetheine 泛酰巯基⼄胺pantothenate 泛酸;泛酸盐、酯、根pantropic virus 泛嗜性病毒papain ⽊⽠蛋⽩酶papaverine 罂粟碱paper raft nursing technique 纸桶保育技术[可⽤于培养单个植物细胞]papilla [植物]乳突⽑;[动物]*papillomavirus *瘤病毒papovavirus 乳多空病毒parabasal body 副基粒paracasein 副酪蛋⽩,衍酪蛋⽩paracentric inversion 臂内倒位parachromatin 副染⾊质paracodon 副密码⼦[tRNA上被氨酰tRNA合成酶识别的碱基,与tRNA识别氨基酸有关]paracrine 旁分泌paracrystal 次晶paracrystalline state 次晶态paradoxical sleep 异相睡眠paraffin imbedding ⽯蜡包埋法Parafilm [商]⽯蜡膜,⽯蜡封⼝膜[American Can公司的商标]paraformaldehyde 低聚甲醛,仲甲醛,多聚甲醛parafuscin 草履⾍融膜蛋⽩paraglobulin 副球蛋⽩paralbumin 副蛋⽩,副清蛋⽩parallel 平⾏的paralogous gene 共⽣同源基因,平⾏进化同源基因paramagnetic 顺磁的paramecin 草履⾍素,草履⾍蛋⽩paramecium 草履⾍paramucin 异粘液素paramucosin 仲唾液蛋⽩paramutation 副突变paramylum 原⽣动物糖paramyosin 副肌球蛋⽩paramyxovirus 副粘病毒paranemic joint 平⾏汇接[由双链DNA分⼦在重组区解旋⽽形成]paranemic spiral 平⾏螺旋,反向双股螺旋pararosaniline 碱性副品红parasexuality 准性⽣殖parasite 寄⽣⾍parasitism 寄⽣parasporal crystal 伴胞晶体parathion 对硫磷parathyrin 甲状旁腺素parathyroid gland 甲状旁腺paratope [抗原]互补位parenchyma [植物]薄壁组织;[动物]实质parental 亲本的,亲代的parental imprinting 亲本印记[配⼦发⽣过程中亲本基因的选择性差异表达]parental type 亲本型[如⽤于描述⼦代性状]parental virus 亲代病毒parity 宇称parkinson disease 帕⾦森病paromomycin 巴龙霉素parotin 腮腺素pars amorpha [核仁]⽆定形区pars fibrosa [核仁]纤维区pars granulosa [核仁]颗粒区parsnip yellow fleck virus 欧防风黄点病毒parthenocarpy 单性结实parthenogamy 孤雌核配parthenogenesis 孤雌⽣殖[雌体产⽣不需受精即可发育的卵⼦];孤雌发育[卵⼦不经受精进⾏发育] parthenogenetic embryo 单性胚,孤雌胚parthenogonidium 孤雌⽣殖细胞parthenomixis 孤雌两核融合partial molar 偏摩尔的particle gun 基因枪,粒⼦枪partitivirus 分病毒parvalbumin ⼩⽩蛋⽩,⼩清蛋⽩[如见于鲤鱼]parvovirus 细⼩病毒passage [细胞]传代passage type 过渡形式Pasteur effect 巴斯德效应,巴⽒效应[有氧氧化抑制酵解]pasteur pipet 巴⽒吸管,巴斯德吸管Pasteurella 巴⽒菌属,巴斯德菌属pasteurization 巴⽒消毒法patch clamp 膜⽚箝,膜⽚钳patch clamping technique 膜⽚箝术,膜⽚钳术[可⽤于监测膜通道活性]patching 膜⽚形成paternity test 亲权认定pathogen 病原体pathovar 致病变型patroclinal ingeritance 偏⽗遗传patrogenesis 孤雄⽣殖pattern [特征序列]模式patulin 展青霉素Pauli exclusion principle 泡利不相容原理pauperization 杂交弱势paxillin 桩蛋⽩[见于粘着斑,被栓在膜上]pea enation mosaic virus 豌⾖⽿突花叶病毒pectamycin 密旋霉素pectin 果胶pectinase 果胶酶pedigree 系谱pediocin ⽚球菌素pellicle 菌膜;(菌)醭;[细胞]表膜penetrance 外显率penicillinase 青霉素酶penicillium 青霉属penicillium chrysogenum virus 产毒青霉病毒pentagastrin 五肽胃泌素pentamer 五聚体penton 五邻体[见于腺病毒]pentosan 戊聚糖pentose 戊糖pentyl 戊基peplomer 包膜突起peplos 包膜pepscan 肽扫描(技术)pepsin 胃蛋⽩酶pepsinogen 胃蛋⽩酶原pepsitensin 胃酶解⾎管紧张肽pepstatin 胃(蛋⽩)酶抑制剂,抑胃酶肽peptidase 肽酶peptide nucleic acid 肽核酸[⼀类DNA类似物,以氨基酸取代糖磷酸主链]peptide screening 肽筛选[常指利⽤合成肽进⾏表位作图的⽅法]peptidergic fiber 肽能纤维peptidoglycan 肽聚糖peptidyl 肽基peptization 胶溶peptone 胨pepzyme 肽性酶[⼈⼯合成的⼩分⼦肽催化剂]Percoll [商]珀可[Pharmacia公司商标,是聚⼄烯吡咯酮包被的⼆氧化硅壳粒的⽆菌胶体悬液,可以形成1.3g/ml以下的各种密度梯度]perforin 穿孔素perfringocin 产⽓荚膜羧菌素perfusion 灌流peri effect 近位效应peri position 近位perianth 花被;[苔藓]蒴萼periblem ⽪层原[见于植物]pericardial cavity ⼼包腔pericardium ⼼包膜pericentric inversion 臂间倒位periclinal 平周的pericycle 中柱鞘periderm 周被[见于植物]peridium [粘菌]孢囊被;包被perikaryon 核周体periodic protein 周期性蛋⽩[含有周期性重复序列]periosteum ⾻外膜peripheral 外周的,周边的peripherin 外周蛋⽩[⼀种中间丝蛋⽩,最初发现于神经元]periplasm (外)周质periplast 周质体perisperm 外胚乳peristalsis 蠕动peristaltic pump 蠕动泵perithecium ⼦囊壳peritoneum 腹膜perlecan 基底膜(蛋⽩)聚糖permeability 通透性permeabilization 透化(作⽤)[使通透性增加]permeabilizing 透化(处理)permease 通透酶permissive action 允许作⽤[如特指激素间⼀种协同作⽤]permselective membrane 选择透性膜,选择(性)通透膜permselectivity 选择通透性permutation 变换,置换;排列peroxidase 过氧化物酶persitol 鳄梨糖醇perturbation 微扰pertussis toxin 百⽇咳毒素pervaporation 全蒸发perxisome 过氧化物酶体pesticin ⿏疫菌素pestivirus 瘟病毒属petri dish 培养⽫petroselinic acid 岩芹酸,6-⼗⼋(碳)烯酸Pfu DNA polymerase Pfu DNA聚合酶[来⾃Pyrococcus furiosus的耐热DNA聚合酶(Stratagene公司专利产品)兼具5'-3-DNA 聚合活性及3'-5'外切校正活性]phaeophyll 叶褐素phaeophyta 褐藻门phaeophytin 褐藻素phaeoplast 叶褐体phage antibody 噬菌体抗体[噬菌体蛋⽩与免疫球蛋⽩的融合体,表达于噬菌体表⾯]phage display 噬菌体展⽰[将抗体或肽表位展⽰于噬菌体表⾯]phage typing 噬菌体分型[利⽤噬菌体进⾏细菌分型]phagecyte 吞噬细胞phagemid 噬菌粒,噬粒phagetype 噬菌体型phagevar 噬菌体变型phagocytosis 吞噬(作⽤)phagosome 吞噬体phallacidin 类⿁笔(毒)环肽phallin ⿁笔溶⾎(毒)环肽,⽩⿁笔(毒)环肽phallisin 类⿁笔素phalloidin ⿁笔(毒)环肽phalloin ⿁笔素phallotoxin ⿁笔毒素,⿁笔毒蕈肽[类名,包括⿁笔素,⿁笔环肽等]pharynx 咽phaseolin 云扁⾖蛋⽩phaseoline 菜⾖碱phaseolotoxin 菜⾖丁⾹假单胞杆菌毒素,菜⾖菌毒素phasmid 噬菌粒,噬粒PhastGel [商]快速凝胶[PhastSystem所⽤现成凝胶]PhastSystem [商]快速凝胶电泳系统[Pharmacia公司⽣产的快速聚丙烯酰胺凝胶电泳]phenanthrene 菲phenanthroline 菲咯啉phenazine 吩嗪phenobarbital 苯巴⽐妥phenocopy 拟表型,表型模拟phenogenetics 发育遗传学phenotype 表型phenotypic 表型的phentolamine 酚妥拉明phenylacetamidase 苯⼄酰胺酶phenylacetamide 苯⼄酰胺phenylacetic acid 苯⼄酸phenylalanini 苯丙氨酸phenylarsenic oxide 氧化苯胂phenylethanol 苯基⼄醇phenylethanolamine 苯基⼄醇胺phenylethylamine 苯⼄胺phenylisothiocyanate 异硫氰酸苯酯phenylketonuria 苯丙酮尿症phenylthiocarbamide 苯硫脲。
密度梯度离心的英文Density Gradient Centrifugation.Density gradient centrifugation is a powerful technique used in biochemistry and molecular biology to separate particles based on their density. This method exploits the difference in density between the particles and the surrounding medium, allowing for the efficient purification and fractionation of complex mixtures. In this article, we will explore the principles, applications, and advantages of density gradient centrifugation.Principles of Density Gradient Centrifugation.Density gradient centrifugation relies on theprinciples of sedimentation and buoyancy. When a particleis placed in a liquid medium, it experiences a force called the sedimentation force, which is proportional to the mass of the particle and the square of the centrifugal force. On the other hand, the buoyancy force, which opposes thesedimentation force, is proportional to the volume of the particle and the density of the medium.In density gradient centrifugation, a sample is layered on top of a gradient medium, which is typically a solution containing substances with gradually increasing density. When centrifuged, the particles in the sample migrate through the gradient medium based on their sedimentation and buoyancy forces. Particles with higher density sediment faster and migrate towards the bottom of the tube, while particles with lower density migrate slower and remain towards the top. This results in the formation of distinct bands within the gradient, each containing particles of similar density.Applications of Density Gradient Centrifugation.Density gradient centrifugation finds applications in various fields of biochemistry and molecular biology. Here are some examples:1. Cell Fractionation: Density gradient centrifugationis commonly used to separate different cellular compartments, such as mitochondria, lysosomes, and peroxisomes. By using gradients of sucrose or other dense media, these organelles can be purified based on their density differences.2. Virus Purification: Density gradient centrifugation is a crucial step in the purification of viruses. Virus particles can be separated from cellular debris and other contaminants by centrifuging them through a gradient of cesium chloride or sucrose. This method allows for the isolation of highly purified virus preparations.3. Protein Purification: Density gradient centrifugation can be employed to purify proteins based on their density. For instance, gradient media such as iodixanol or percoll can be used to separate proteins from each other or from contaminants. This technique is especially useful in purifying proteins from complex mixtures, such as cell lysates or serum.4. Nucleic Acid Purification: Density gradientcentrifugation is also used to purify nucleic acids, such as DNA and RNA. By centrifuging nucleic acid samples through gradients of cesium chloride or other dense media, impurities can be removed, and the nucleic acids can be recovered in high purity.Advantages of Density Gradient Centrifugation.Density gradient centrifugation offers several advantages over other separation techniques:1. High Resolution: Density gradient centrifugation allows for the separation of particles with closely related densities. The gradual increase in density within the gradient medium provides a continuous separation environment, enabling the formation of distinct bands even for particles with slight differences in density.2. Gentle Separation: Compared to other centrifugation techniques, density gradient centrifugation is relatively gentle on the particles being separated. The gradual density change within the gradient minimizes the shearforces acting on the particles, reducing the risk of damage or aggregation.3. High Purity: Density gradient centrifugation can achieve high purity separations, as the particles migrate through the gradient based solely on their density. This minimizes the co-sedimentation of contaminants and allows for the isolation of highly purified fractions.4. Scalability: Density gradient centrifugation can be scaled up or down depending on the sample volume and the desired resolution. This flexibility allows for the separation of both small and large samples, making it suitable for a wide range of applications.Conclusion.Density gradient centrifugation is a powerful technique for separating particles based on their density. By exploiting the principles of sedimentation and buoyancy, it allows for the efficient purification and fractionation of complex mixtures. With its high resolution, gentleseparation, and high purity, density gradient centrifugation finds applications in various fields of biochemistry and molecular biology, including cell fractionation, virus purification, protein purification, and nucleic acid purification.。
表面等离子体共振英文Surface plasmon resonance (SPR) is a phenomenon that occurs when polarized light hits a metal-dielectric interface at a specific angle, causing the electrons on the metal surface to oscillate in resonance with the light wave. This interaction leads to the generation of surface plasmons, which are coherent delocalized electron oscillations that exist at the interface between two materials where the real part of the dielectric function changes sign across the interface.The significance of SPR lies in its sensitivity to changes in the refractive index of the material close to the metal surface. This sensitivity makes SPR an invaluable tool in various fields, particularly in biosensing, where it is used to detect the binding of molecules to the metal surface. The binding event causes a change in the refractive index at the surface, which in turn alters the resonance condition. By measuring this change, one can infer details about the molecular interaction, such as the binding kinetics and affinity.In a typical SPR experiment, a thin metal film, usually gold or silver, is deposited on a glass substrate. The metal film is then exposed to a polarized light source, and the angle of incidence is varied until the resonance condition is met. At resonance, there is a significant reduction in the reflected light intensity, which is detected by a photodetector. The angle at which this dip in reflectivity occurs is referred to as the resonance angle and is highly sensitive to the refractive index of the material in contact with the metal film.The applications of SPR are vast and diverse. In the field of biochemistry, it is used to study protein-protein interactions, DNA hybridization, and the binding of small molecules to proteins. In environmental monitoring, SPR sensors can detect the presence of pollutants and pathogens. The technology is also employed in the pharmaceutical industry for drug discovery and the characterization of biomolecular interactions.One of the key advantages of SPR is that it allows for real-time monitoring of binding events without the need for labeling the interacting molecules. This non-invasivenature preserves the biological activity of the molecules and provides a more accurate representation of the interaction as it occurs in vivo.Recent advancements in SPR technology have led to the development of localized SPR (LSPR), which operates on the same principles but at a much smaller scale. LSPR is associated with nanostructures, such as nanoparticles, and offers enhanced sensitivity and spatial resolution. This miniaturization has opened up new possibilities for the integration of SPR sensors into microfluidic systems and the potential for high-throughput analysis.In conclusion, surface plasmon resonance is a powerful analytical technique that has revolutionized the way we study and understand molecular interactions. Its ability to provide real-time, label-free analysis makes it an indispensable tool in scientific research and various industries. As technology continues to advance, we can expect SPR to play an even more significant role in the fields of biosensing, environmental monitoring, and beyond.。
光谱层英文版The Spectral Layer: Unveiling the Invisible RealmThe universe we inhabit is a tapestry of intricately woven elements, each thread contributing to the grand tapestry of existence. Amidst this intricate web, lies a realm that is often overlooked, yet holds the key to unlocking the mysteries of our reality. This realm is the spectral layer – a realm that transcends the boundaries of our visible world and delves into the unseen realms of energy and vibration.At the heart of the spectral layer lies the electromagnetic spectrum –a vast and diverse range of wavelengths and frequencies that encompass the entirety of our physical world. From the low-frequency radio waves to the high-energy gamma rays, the electromagnetic spectrum is the foundation upon which our understanding of the universe is built. It is within this spectrum that we find the familiar visible light, the spectrum of colors that we perceive with our eyes, but it is only a small fraction of the vast and diverse tapestry that makes up the spectral layer.Beyond the visible spectrum, there lies a realm of unseen energies that are integral to the very fabric of our existence. Infrared radiation, for instance, is a form of electromagnetic radiation that is invisible to the human eye but plays a crucial role in the transfer of heat and the functioning of various biological processes. Similarly, ultraviolet radiation, though invisible to us, is essential for the production of vitamin D and the regulation of circadian rhythms.But the spectral layer extends far beyond the confines of the electromagnetic spectrum. It is a realm that encompasses the vibrations and frequencies of all matter and energy, from the subatomic particles that make up the building blocks of our universe to the vast cosmic structures that span the vastness of space. These vibrations and frequencies, though often imperceptible to our senses, are the foundation upon which the entire universe is built.At the quantum level, the spectral layer reveals the true nature of reality. Subatomic particles, such as electrons and quarks, are not merely static entities but rather dynamic oscillations of energy, each with its own unique frequency and vibration. These vibrations, in turn, give rise to the fundamental forces that govern the behavior of matter and energy, from the strong nuclear force that holds the nucleus of an atom together to the mysterious dark energy that drives the expansion of the universe.But the spectral layer is not merely a realm of the infinitely small. It also encompasses the vast and expansive structures of the cosmos, from the intricate patterns of galaxies to the pulsing rhythms of celestial bodies. The stars that dot the night sky, for instance, are not merely points of light but rather vast nuclear furnaces, each emitting a unique spectrum of electromagnetic radiation that can be detected and analyzed by scientists.Through the study of the spectral layer, we have gained unprecedented insights into the nature of our universe. By analyzing the spectra of distant galaxies, for example, we can determine their chemical composition, their age, and even their rate of expansion –information that is crucial for our understanding of the origins and evolution of the cosmos.But the spectral layer is not just a realm of scientific inquiry – it is also a realm of profound spiritual and metaphysical exploration. Many ancient and indigenous cultures have long recognized the importance of the unseen realms of energy and vibration, and have developed sophisticated systems of understanding and interacting with these realms.In the traditions of Hinduism and Buddhism, for instance, the concept of the chakras – the seven energy centers that are believed to govern various aspects of our physical, emotional, and spiritualwell-being – is a manifestation of the spectral layer. These energy centers are believed to be connected to specific frequencies and vibrations, and the practice of chakra meditation and balancing is seen as a way to align oneself with the natural rhythms of the universe.Similarly, in the traditions of shamanism and indigenous healing practices, the concept of the "spirit world" or the "unseen realm" is closely tied to the spectral layer. Shamans and healers are often said to be able to perceive and interact with the unseen energies that permeate our world, using techniques such as drumming, chanting, and plant medicine to access these realms and bring about healing and transformation.In the modern era, the spectral layer has become the subject of intense scientific and technological exploration. From the development of advanced imaging technologies that can reveal the unseen structures of the human body to the creation of sophisticated communication systems that harness the power of the electromagnetic spectrum, the spectral layer has become an essential component of our understanding and manipulation of the physical world.Yet, despite the immense progress we have made in our understanding of the spectral layer, there is still much that remainsunknown and mysterious. The nature of dark matter and dark energy, for instance, remains one of the greatest unsolved puzzles in modern physics, and the true nature of consciousness and the relationship between the physical and the metaphysical realms continues to be a subject of intense debate and exploration.As we continue to delve deeper into the spectral layer, we may uncover even more profound insights into the nature of our reality. Perhaps we will discover new forms of energy and vibration that have yet to be detected, or perhaps we will find that the boundaries between the seen and the unseen are far more permeable than we ever imagined. Whatever the future may hold, one thing is certain: the spectral layer will continue to be a source of fascination, inspiration, and mystery for generations to come.。
中文英文色谱图chromatogram色谱峰chromatographic peak峰底peak base峰高h,peak height峰宽W,peak width半高峰宽Wh/2,peak width at half height峰面积A,peak area拖尾峰tailing area前伸峰leading area假峰ghost peak畸峰distorted peak反峰negative peak拐点inflection point原点origin斑点spot区带zone复班multiple spot区带脱尾zone tailing基线base line基线漂移baseline drift基线噪声N,baseline noise统计矩moment一阶原点矩γ1,first origin moment二阶中心矩μ2,second central moment三阶中心矩μ3,third central moment液相色谱法liquid chromatography,LC液液色谱法liquid liquid chromatography,LLC液固色谱法liquid solid chromatography,LSC正相液相色谱法normal phase liquid chromatography反相液相色谱法reversed phase liquid chromatography,RPLC 柱液相色谱法liquid column chromatography高效液相色谱法high performance liquid chromatography,HPLC 尺寸排除色谱法size exclusion chromatography,SEC凝胶过滤色谱法gel filtration chromatography凝胶渗透色谱法gel permeation chromatography,GPC亲和色谱法affinity chromatography离子交换色谱法ion exchange chromatography,IEC离子色谱法ion chromatography离子抑制色谱法ion suppression chromatography离子对色谱法ion pair chromatography疏水作用色谱法hydrophobic interaction chromatography制备液相色谱法preparative liquid chromatography平面色谱法planar chromatography纸色谱法paper chromatography薄层色谱法thin layer chromatography,TLC高效薄层色谱法high performance thin layer chromatography,HPTLC 浸渍薄层色谱法impregnated thin layer chromatography凝胶薄层色谱法gel thin layer chromatography离子交换薄层色谱法ion exchange thin layer chromatography制备薄层色谱法preparative thin layer chromatography薄层棒色谱法thin layer rod chromatography液相色谱仪liquid chromatograph制备液相色谱仪preparative liquid chromatograph凝胶渗透色谱仪gel permeation chromatograph涂布器spreader点样器sample applicator色谱柱chromatographic column棒状色谱柱monolith column monolith column微粒柱microparticle column填充毛细管柱packed capillary column空心柱open tubular column微径柱microbore column混合柱mixed column组合柱coupled column预柱precolumn保护柱guard column预饱和柱presaturation column浓缩柱concentrating column抑制柱suppression column薄层板thin layer plate浓缩区薄层板concentrating thin layer plate荧光薄层板fluorescence thin layer plate反相薄层板reversed phase thin layer plate梯度薄层板gradient thin layer plate烧结板sintered plate展开室development chamber往复泵reciprocating pump注射泵syringe pump气动泵pneumatic pump蠕动泵peristaltic pump检测器detector微分检测器differential detector积分检测器integral detector总体性能检测器bulk property detector溶质性能检测器solute property detector(示差)折光率检测器[differential] refractive index detector荧光检测器fluorescence detector紫外可见光检测器ultraviolet visible detector电化学检测器electrochemical detector蒸发(激光)光散射检测器[laser] light scattering detector光密度计densitometer薄层扫描仪thin layer scanner柱后反应器post-column reactor体积标记器volume marker记录器recorder积分仪integrator馏分收集器fraction collector工作站work station固定相stationary phase固定液stationary liquid载体support柱填充剂column packing化学键合相填充剂chemically bonded phase packing薄壳型填充剂pellicular packing多孔型填充剂porous packing吸附剂adsorbent离子交换剂ion exchanger基体matrix载板support plate粘合剂binder流动相mobile phase洗脱(淋洗)剂eluant,eluent展开剂developer等水容剂isohydric solvent改性剂modifier显色剂color [developing] agent死时间t0,dead time保留时间tR,retention time调整保留时间t'R,adjusted retention time死体积V0,dead volume保留体积vR,retention volume调整保留体积v'R,adjusted retention volume柱外体积Vext,extra-column volune粒间体积V0,interstitial volume(多孔填充剂的)孔体积VP,pore volume of porous packing 液相总体积Vtol,total liquid volume洗脱体积ve,elution volume流体力学体积vh,hydrodynamic volume相对保留值ri.s,relative retention value分离因子α,separation factor流动相迁移距离dm,mobile phase migration distance流动相前沿mobile phase front溶质迁移距离ds,solute migration distance比移值Rf,Rf value高比移值hRf,high Rf value相对比移值Ri.s,relative Rf value保留常数值Rm,Rm value板效能plate efficiency折合板高hr,reduced plate height分离度R,resolution液相载荷量liquid phase loading离子交换容量ion exchange capacity负载容量loading capacity渗透极限permeability limit排除极限Vh,max,exclusion limit拖尾因子T,tailing factor柱外效应extra-column effect管壁效应wall effect间隔臂效应spacer arm effect边缘效应edge effect斑点定位法localization of spot放射自显影法autoradiography原位定量in situ quantitation生物自显影法bioautography归一法normalization method内标法internal standard method外标法external standard method叠加法addition method普适校准(曲线、函数) calibration function or curve [function]谱带扩展(加宽) band broadening(分离作用的)校准函数或校准曲线universal calibration function or curve [of separation] 加宽校正broadening correction加宽校正因子broadening correction factor溶剂强度参数ε0,solvent strength parameter洗脱序列eluotropic series洗脱(淋洗) elution等度洗脱gradient elution梯度洗脱gradient elution(再)循环洗脱recycling elution线性溶剂强度洗脱linear solvent strength gradient程序溶剂programmed solvent程序压力programmed pressure程序流速programmed flow展开development上行展开ascending development下行展开descending development双向展开two dimensional development 环形展开circular development离心展开centrifugal development向心展开centripetal development径向展开radial development多次展开multiple development分步展开stepwise development连续展开continuous development梯度展开gradient development匀浆填充slurry packing停流进样stop-flow injection阀进样valve injection柱上富集on-column enrichment流出液eluate柱上检测on-column detection柱寿命column life柱流失column bleeding显谱visualization活化activation反冲back flushing脱气degassing沟流channeling过载overloading。
Note on Breakup Densities in FragmentationV. E. ViolaIUCF and Department of ChemistryIndiana UniversityBloomington, IN 47408In [1] the breakup density of hot nuclei as a function of excitation energy E*/A was derived from analysis of kinetic-energy spectra for intermediate-mass fragments ( IMF: 2<Z~20 ) emitted in light-ion induced reactions on 197Au nuclei. The results indicated a breakup density that decreases from normal density ρo at excitation energies below E*/A ~ 2 MeV to a value of ρ/ρο ∼ 0.3 for Ε∗/Α ∼ 5 ΜeV and above. This analysis has been questioned [2,3] on the grounds that a parameterization based on a sequential emission model [4] was used to fit the spectra, seemingly in conflict with the observation that the time scale is nearly simultaneous above E*/A ~ 3 MeV. The purpose of this note is to elaborate on the assumptions that were employed in [1] and to stress that the sequential emission formalism of [4] served only as a spectral fitting function, independent of time scale. The analysis in [1] was prompted by the observed systematic decrease in the IMF spectral “Coulomb” peaks with increasing excitation energy [6,7], contrary to the expected increase with the higher temperature of the emitting system. Two plausible explanations for the observed behavior are (1) a decrease in source charge due to fast cascade/preequilibrium charge loss prior to thermalization, and (2) a decrease in density due to expansion/dilution of the emitting source. The source charge can be corrected from the data, since the nonequilibrium particles were measured experimentally [8]. The extent of expansion/dilution is reflected by the separation distance between a fragment and the Coulomb field generated by the ensemble of remaining particles. Using Coulomb’s law, this distance can be derived from the fragment kinetic energy spectra, as described below.Our analysis is first-order and descriptive of an average process. For high multiplicity events the measured spatial patterns of the fragments involve a broad distribution of configurations that can only be addressed collectively. In addition, an effort was made to favor maximum breakup densities whenever ambiguities in the procedure occurred. The principal assumptions for the disintegrating system are as follows: •The average breakup configuration is isotropic, as has been indicated by a sphericity/coplanarity analysis [9]. Fluctuations in the event topology are assumed to be reflected in the widths of the spectra.•Only equilibrium-like particles are included in the fitting procedure and nonequilibrium particles are subtracted from the target charge to determine the source charge. (This procedure agrees well with the results of the EOS collaboration [10]).•Fragment acceleration is governed only by the average Coulomb field between the an IMF and the residual system; i.e. there is no significant radial flow [11], although this possibility is also addressed in[1].•From a knowledge of the IMF kinetic energy distributions and the charges of the IMF and the residue, the average separation distance can be extracted, defining the breakup volume for a spherical system. Thus, the problem is reduced to one of relating the IMF kinetic energy spectra to some average separation distance and finding an appropriate normalization to ρo.The spectral analysis in [1] is analogous to that employed in the derivation of fission-fragment kinetic-energy systematics, from which fragment-fragment charge separation distances can be derived [12]. The principal difference is that the functional dependence in [1] is on E*/A instead of Z2/A1/3 as in [12]. At moderateexcitation energies the mass division in fission is symmetric, leading to fragment kinetic energy distributions that are Gaussian-like and thus uniquely characterized. The effect of excitation energy is reflected only in the widths of the distributions [13]. In contrast, IMF emission is asymmetric and the kinetic-energy distributions are Maxwellian in shape – whether in binary emission or multifragmentation. This leads to several possible ways to describe the shifts in the spectral peaks.In order to describe the spectral shifts, the choice of the Coulomb parameter from the Moretto model [4], as modified by Kwiatkowski [14], was dictated by practical considerations. Most important was that the Coulomb parameters had been previously obtained in moving-source fits that were performed in order to separate equilibrium and nonequilibrium emissions, determine source velocities, and compare slope temperatures with Fermi-gas expectations. Specific features included the following:•When the separation distances based on fission fragment kinetic-energy systematics are used for the radius parameter in the model, excellent fits to the spectra for binary emission at normal density areobtained [7]. This assumption provided our normalization to normal density.•The program contained the kinematic factors required to assure consistency in the source frame transformations.•The model allowed for the observed broadening of the spectral widths with increasing E*/A due to thermal and fragment deformation effects.•Corrections to the source charge were applied to account for mass loss due to nonequilibrium emission. This approach allowed us to fit hundreds of spectra in order to obtain systematic Coulomb parameters, source velocities and slope temperatures as a function of both IMF charge and E*/A. Nowhere in the analysis is the assumption of sequential emission used. Although much earlier we pointed out the qualitative link between the decreasing Coulomb parameters and the breakup density, the quantitative analysis in [1] was a light that snapped on much later.It should be stressed that we could have chosen any number of metrics for fitting the IMF kinetic-energy spectra -- e.g. the most probable, average, or centroid at FWHM of the kinetic energy distributions. The results would not be significantly different than in [1], although more poorly defined. Some concern exists that the breakup densities in [1] are somewhat lower than those derived from caloric curves by Natowitz [15], derived largely from heavy-ion data. Possible sources for the difference may reside in the compression/expansion energy and/or rotational effects that may enhance breakup at a somewhat higher density than in light-ion-induced reactions. In addition, the reaction dynamics of GeV light-ion reactions indicate that the nucleus is formed in a relatively dilute state due to multiple knockout reactions during the fast cascade that initiates the energy deposition process [16].One final note on this analysis. The densities quoted in [1] are based on an average of values for individual IMFs from Z = 4-10. Closer examination of results for individual IMFs reveals a trend in which the breakup density increases as the IMF charge decreases, such that for He ions the breakup density is close to normal density. However, within experimental errors, this effect is only suggestive.References1)V.E. Viola, K. Kwiatkowski, J.B. Natowitz and S. J. Yennello, Phys. Rev. Lett. 93, (2004) 132701.2)Ad. Raduta et al, Phys. Lett. B 623 (2005) 43.3)S.K. Samaddar, J.N. De, X. Vinas and M. Centelles, arXiv:nucl-th/0701072v1, Jan. (2007).4)L.G. Moretto, Nucl. Phys.A 247, (1975) 211.5)L. Beaulieu et al, Phys. Rev. Lett. 84 (2000) 5971.6) D.S. Bracken et al, Phys. Rev. C 69 (2004) 034612.7)J.L. Wile et al, Phys. Rev. C 45 (1992) 2300.8)T. Lefort et al, Phys. Rev. C 64 (2001) 064603.9) E. Renshaw Foxford et al, Phys. Rev. C 54 (1996) 749.10) J. Hauger et al, Phys. Rev. C 62 (2000) 024616 and references therein.11) T. Lefort et al, Phys. Rev. C 62 (2000) 031604 (R).12) V. E. Viola and T. Sikkeland, Phys. Rev. 130 (1963) 2044.13) J. R. Nix and W.J. Swiatecki, Nucl. Phys. 71 (1965) 114) K. Kwiatkowski, Phys. Lett. B 171, (1986) 4115) J. B. Natowitz et al, Phys. Rev. C 65 (2002) 034618.16) S. Turbide, P. Danielewicz et al, Phys. Rev. C 70 (2004) 014608.。
Chapter 1Downstream processing(DSP):The isolation and purification of a biotechnological product to a form suitable for its intended use. The separation and purification of products synthesized by bioprocesses:Biotechnology:the use of cultured microorganisms, animal cells, and plant cells to produce products useful to humans.Modern biotechnology:Built on genetic engineering to produce commercial products or processes.Chapter 2Coagulation:the chemical alteration of the colloidal particles to make them stick together凝聚值:表示电解质的凝聚能力,使胶粒发生凝聚作用的最小电解质浓度m mol/L. Flocculation: a process whereby particles are aggregated into clusters.Filtration separates solid from a liquid by forcing the liquid through a filter medium.滤浆(feed/ slurry):悬浮液过滤介质(filter medium) :多孔物质滤液(filtrate):通过过滤介质的液体滤饼(filter cake):被截留的固体物质Conventional or dead-end filtration: the fluid flows perpendicular to the medium which result in a cake of solids depositing on the filter medium.Crossflow filtration:The fluid flows parallel to the medium to minimize buildup to solids on the medium.Centrifugation is a process that involves the use of the centrifugal force for the separation of mixtures.分离因数(Z):离心力与重力的比值。
高分子材料工程专业英语词汇及部分课文翻译------------------------------------------作者------------------------------------------日期专业英语词汇accordion 手风琴 activation 活化(作用)addition polymer 加成聚合物,加聚物 aggravate 加重,恶化 agitation 搅拌 agrochemical 农药,化肥 Alfin catalyst 醇(碱金属)烯催化剂 align 排列成行 aliphatic 脂肪(族)的 alkali metal 碱金属 allyl 烯丙基aluminum alkyl 烷基铝 amidation 酰胺化(作用) amino 氨基,氨基的 amorphous 无定型的,非晶体的 anionic 阴(负)离子的 antioxidant 抗氧剂 antistatic agent 抗静电剂 aromatic 芳香(族)的 arrangement (空间)排布,排列 atactic 无规立构的 attraction 引力,吸引 backbone 主链,骨干 behavior 性能,行为 biological 生物(学)的 biomedical 生物医学的bond dissociation energy 键断裂能 boundary 界限,范围 brittle 脆的,易碎的 butadiene 丁二烯 butyllithium 丁基锂 calendering 压延成型 calendering 压延 carboxyl 羧基 carrier 载体catalyst 催化剂,触媒 categorization 分类(法) category 种类,类型 cation 正[阳]离子cationic 阳(正)离子的 centrifuge 离心 chain reaction 连锁反应 chain termination 链终止 char 炭 characterize 表征成为…的特征 chilled water 冷冻水 chlorine 氯(气) coating 涂覆 cocatalyst 助催化剂 coil 线团 coiling 线团状的 colligative 依数性 colloid 胶体 commence 开始,着手 common salt 食盐 complex 络合物 compliance 柔量 condensation polymer 缩合聚合物,缩聚物conductive material 导电材料 conformation 构象 consistency 稠度,粘稠度 contaminant 污物 contour 外形,轮廓controlled release 控制释放 controversy 争论,争议 conversion 转化率 conversion 转化 copolymer 共聚物 copolymerization 共聚(合) corrosion inhibitor 缓释剂 countercurrent 逆流 crosslinking 交联 crystal 基体,结晶 crystalline 晶体,晶态,结晶的,晶态的crystalline 结晶的 crystallinity 结晶性,结晶度 crystallite 微晶 decomposition 分解 defect 缺陷 deformability 变形性,变形能力 deformation 形变 deformation 变形degree of polymerization 聚合度 dehydrogenate 使脱氢 density 密度depolymerization 解聚 deposit 堆积物,沉积 depropagation 降解 dewater 脱水diacid 二(元)酸 diamine 二(元)胺 dibasic 二元的 dieforming 口模成型 diffraction 衍射 diffuse 扩散 dimension 尺寸 dimensional stability 尺寸稳定性 dimer 二聚物(体) diol 二(元)醇 diolefin 二烯烃 disintegrate 分解,分散,分离 dislocation 错位,位错 dispersant 分散剂 dissociate 离解 dissolution 溶解dissolve 使…溶解distort 使…变形,扭曲 double bond 双键dough (生)面团,揉好的面 drug 药品,药物elastic modulus 弹性模量 elastomer 弹性体 eliminate 消除,打开,除去 elongation 伸长率,延伸率 entanglement 缠结,纠缠 entropy 熵 equilibrium 平衡 esterification 酯化(作用) evacuate 撤出 extrusion 注射成型 extrusion 挤出 fiber 纤维flame retardant 阻燃剂 flexible 柔软的flocculating agent 絮凝剂folded-chain lamella theory 折叠链片晶理论 formulation 配方 fractionation 分级 fragment 碎屑,碎片 fringed-micelle theory 缨状微束理论 functional group 官能团 functional polymer 功能聚合物 functionalized polymer 功能聚合物 gel 凝胶glass transition temperature 玻璃化温度 glassy 玻璃(态)的 glassy 玻璃态的 glassy state 玻璃态 globule 小球,液滴,颗粒 growing chain 生长链,活性链 gyration 旋转,回旋 hardness 硬度 heat transfer 热传递 heterogeneous 不均匀的,非均匀的 hydocy acid 羧基酸 hydrogen 氢(气) hydrogen bonding 氢键 hydrostatic 流体静力学 hydroxyl 烃基 hypothetical 假定的,理想的,有前提的 ideal 理想的,概念的 imagine 想象,推测imbed 嵌入,埋入,包埋 imperfect 不完全的 improve 增进,改善 impurity 杂质 indispensable 不了或缺的 infrared spectroscopy 红外光谱法 ingredient 成分 initiation (链)引发 initiator 引发剂inorganic polymer 无机聚合物 interaction 相互作用 interchain 链间的interlink 把…相互连接起来连接 intermittent 间歇式的 intermolecular (作用于)分子间的 intrinsic 固有的 ion 离子ion exchange resin 离子交换树脂 ionic 离子的 ionic polymerization 离子型聚合 irradiation 照射,辐射 irregularity 不规则性,不均匀的 isobutylene 异丁烯 isocyanate 异氰酸酯 isopropylate 异丙醇金属,异丙氧化金属isotactic 等规立构的 isotropic 各项同性的 kinetic chain length 动力学链长 kinetics 动力学 latent 潜在的light scattering 光散射 line 衬里,贴面 liquid crystal 液晶macromelecule 大分子,高分子 matrix 基体,母体,基质,矩阵 mean-aquare end-to-end distance 均方末端距mechanical property 力学性能,机械性能mechanism 机理medium 介质中等的,中间的 minimise 最小化 minimum 最小值,最小的 mo(u)lding 模型 mobility 流动性 mobilize 运动,流动 model 模型 modify 改性molecular weight 分子量 molecular weight distribution 分子量分布molten 熔化的monofunctional 单官能度的 monomer 单体 morphology 形态(学) moulding 模塑成型 neutral 中性的 nonelastic 非弹性的nuclear magnetic resonance 核磁共振 nuclear track detector 核径迹探测器 number average molecular weight 数均分子量occluded 夹杂(带)的 olefinic 烯烃的optimum 最佳的,最佳值[点,状态] orient 定向,取向 orientation 定向 oxonium 氧鎓羊 packing 堆砌 parameter 参数 parison 型柸pattern 花纹,图样式样 peculiarity 特性 pendant group 侧基 performance 性能,特征 permeability 渗透性pharmaceutical 药品,药物,药物的,医药的phenyl sodium 苯基钠 phenyllithium 苯基锂 phosgene 光气,碳酰氯 photosensitizer 光敏剂 plastics 塑料 platelet 片晶 polyamide 聚酰胺 polybutene 聚丁烯polycondensation 缩(合)聚(合) polydisperse 多分散的 polydispersity 多分散性polyesterification 聚酯化(作用) polyethylene 聚乙烯 polyfunctional 多官能度的 polymer 聚合物【体】,高聚物 polymeric 聚合(物)的 polypropylene 聚苯烯 polystyrene 聚苯乙烯 polyvinyl alcohol 聚乙烯醇 polyvinylchloride 聚氯乙烯 porosity 多孔性,孔隙率 positive 正的,阳(性)的 powdery 粉状的 processing 加工,成型 purity 纯度 pyrolysis 热解 radical 自由基radical polymerization 自由基聚合 radius 半径 random coil 无规线团 random decomposition 无规降解 reactent 反应物,试剂reactive 反应性的,活性的 reactivity 反应性,活性 reactivity ratio 竞聚率 real 真是的 release 解除,松开 repeating unit 重复单元 retract 收缩 rubber 橡胶 rubbery 橡胶态的 rupture 断裂 saturation 饱和 scalp 筛子,筛分 seal 密封secondary shaping operation 二次成型 sedimentation 沉降(法) segment 链段 segment 链段semicrystalline 半晶 settle 沉淀,澄清 shaping 成型 side reaction 副作用 simultaneously 同时,同步 single bond 单键 slastic parameter 弹性指数 slurry 淤浆 solar energy 太阳能 solubility 溶解度 solvent 溶剂 spacer group 隔离基团 sprinkle 喷洒 squeeze 挤压srereoregularity 立构规整性【度】 stability 稳定性 stabilizer 稳定剂 statistical 统计的step-growth polymerization 逐步聚合 stereoregular 有规立构的,立构规整性的stoichiometric 当量的,化学计算量的 strength 强度stretch 拉直,拉长 stripping tower 脱单塔 subdivide 细分区分 substitution 取代,代替 surfactant 表面活性剂 swell 溶胀 swollen 溶胀的 synthesis 合成 synthesize 合成 synthetic 合成的tacky (表面)发粘的 ,粘连性 tanker 油轮,槽车tensile strength 抗张强度 terminate (链)终止tertiary 三元的,叔(特)的tetrahydrofuran 四氢呋喃 texture 结构,组织 thermoforming 热成型 thermondynamically 热力学地 thermoplastic 热塑性的 thermoset 热固性的three-dimensionally ordered 三维有序的 titanium tetrachloride 四氯化钛 titanium trichloride 三氯化铁 torsion 转矩transfer (链)转移,(热)传递 triethyloxonium-borofluoride 三乙基硼氟酸羊trimer 三聚物(体)triphenylenthyl potassium 三苯甲基钾 ultracentrifugation 超速离心(分离) ultrasonic 超声波 uncross-linked 非交联的 uniaxial 单轴的 unsaturated 不饱和的 unzippering 开链 urethane 氨基甲酸酯 variation 变化,改变 vinyl 乙烯基(的) vinyl chloride 氯乙烯 vinyl ether 乙烯基醚 viscoelastic 黏弹性的 viscoelastic state 黏弹态 viscofluid state 黏流态 viscosity 黏度viscosity average molecular weight 黏均分子量viscous 粘稠的 vulcanization 硫化weight average molecular weight 重均分子量X-ray x射线 x光 yield 产率Young's modulus 杨氏模量课文翻译第一单元什么是高聚物?什么是高聚物?首先,他们是合成物和大分子,而且不同于低分子化合物,譬如说普通的盐。
1、覆盖层(coverage):描述完全无规则二维网状结构的一个概念,是指一定面积A上的纤维根数N,平均覆盖层C则指纸平面上任意一点的纤维平均层数。
通常也可以只被纤维覆盖的那一部分面积。
C=N.Lf.Wf/A=b/Bf,其中,.Lf.Wf分别为纤维的长度和宽度,b为纸张定量,Bf为纤维的定量,指将纤维单根排列而形成的单层纤维纸页的定量,N是单层排布时所有的纤维总数,A是测定面积。
2、相对键接面积(RBA):总键接面积对于可用于键接的总表面面积之比。
它不可能是100%,通常用来描述纸页的结合度。
3、纸张的匀度(Formation):在一定面积的纸张上,纸张的质量和定量的真实分布状况。
指在纸页平面内小规模定量的波动,是颗粒不均匀分布的结果。
(部分取决于单根纤维沉积内在的随机性,部分取决于纤维的相互作用)4、纤维定向排列(Fiber Orientation):机制纸的一个结构特点,纸页结构的各项异性,纸机方向排列的纤维和垂直纸机方向排列的纤维。
直接影响纸的平面机械性能、尺寸稳定性。
5、纤维定量:单位面积单层纤维层的纤维的质量,可表示为g/cm2(basis weight of fibers)6、(Hydrodynamic smoothing)流体动力滤波:指的是悬浮液在脱水过程中能够改善匀度,在纤维层的最低定量区域内,通过沉积的纤维层流速最高,流动阻力小。
因此,悬浮液流向定量低的地方,这种机理就是流体动力学滤波。
7、Jentzen effect:指从未干燥过的纤维,如果在干燥过程中对其施加轴向拉力,则干燥后其弹性模量和抗张强度会增大,而伸长率减小,如果施加轴向的压缩力,则效果相反,能够解释什么样的干燥条件会改变纤维特性。
8、MD:纸和纸板的纵向,即为纸机运行的方向。
CD:纸和纸板的横向,即为垂直于纸机运行的方向。
9、Density/bulk:(紧度/松厚度):紧度是指单位体积纸或纸板的质量,以g/cm3或kg/m3。
a r X i v :h e p -p h /0102119v 1 9 F eb 2001DCPT/01/12DFTT 1/2001INFNCA-TH0101IPPP/01/06Parton Densities and Fragmentation Functions from Polarized ΛProduction in Semi-Inclusive DISM.Anselmino 1,M.Boglione 2,U.D’Alesio 3,E.Leader 4,∗,F.Murgia 31Dipartimento di Fisica Teorica,Universit`a di Torino and INFN,Sezione di Torino,Via P.Giuria 1,I-10125Torino,Italy2Department of Physics,University of Durham,Science Laboratories,South Road,Durham DH13LE,United Kingdom3INFN,Sezione di Cagliari and Dipartimento di Fisica,Universit`a di Cagliari,C.P.170,I-09042Monserrato (CA),Italy4Physics Department,Theory Division,Vrije Universiteit Amsterdam,De Boelelaan 1081,1081HV Amsterdam,The NetherlandsWe consider the longitudinal polarization of Λand ¯Λproduced in the cur-rent fragmentation region of polarized deep inelastic scattering.We show how the various cross sections can be used to test the underlying parton dynamics,and how one can extract information about certain parton densities which are poorly known,in particular the polarized strange density sum ∆s (x )+∆¯s (x ),and about fragmentation functions which are totally unknown and which are difficult to access by other means.We show also how one can obtain informa-tion concerning the intriguing question as to whether s (x )=¯s (x )and whether ∆s (x )=∆¯s (x ).PACS numbers:13.60.Hb,13.85.Ni,13.87.Fh,13.88.+eI.INTRODUCTIONAs has been emphasized in several papers [1–10],measurements of the polarization of Λbaryons produced in high energy deep inelastic lepton-hadron collisions offer an excellent test of the dynamics of spin transfer from partons to hadrons.In this paper we consider all possible semi-inclusive reactions involving unpolarized or longitudinally polarized leptons and nucleons,with or without the measurement of the lon-gitudinal polarization of Λor ¯Λproduced in the current fragmentation region.We draw theattention to another important aspect of such reactions,namely the information obtainable about the polarized parton densities,and about the unpolarized and polarized fragmentation functions DΛq,∆DΛq for a quark into aΛ(or¯Λ).Despite recent progress[11]some polarized parton densities are still relatively poorly determined.In principle,in semi-inclusive DIS, one can obtain information about the polarized strange quark density∆s(x)+∆¯s(x),which is poorly known,and also about the interesting question as to whether s(x)=¯s(x)and ∆s(x)=∆¯s(x).Regarding the fragmentation functions DΛq and∆DΛq very little is known.Indeed the ∆DΛq are not constrained at all by the present e+e−data.These can,in principle,all be determined in semi-inclusive DIS.They could also be accessed in the reaction pp→ΛX with a polarized proton beam or target[12].In this paper,as in[1],we work in LO QCD.Given the preliminary state of experiments in thisfield it does not seem sensible at this point to undertake the extremely complicated NLO analysis[4]or the somewhat simpler version given in[13].However,as emphasized in[13], it is important to remain vigilant about inaccuracies caused by using the LO formalism,and great attention should be paid to the various tests of the reliability of the LO treatment given in the following.For a more general discussion of this question and suggestions concerning the estimation of theoretical errors generated by the LO treatment,see Ref.[13].To really extract the maximum of information from these reactions one should try to study the triply-differential cross section dσ/dxdydz where x,y,z are the usual semi-inclusive DIS variables[1].In this it is the y-dependence that tests the dynamics,whereas the parton densities and fragmentation functions emerge from the x and z-dependence.In Section II we define precisely what cross sections and polarizations we wish to consider. As mentioned we deal only with longitudinal(helicity)polarization of the leptons,nucleons andΛ’s.In Section III we introduce modified differential cross sections which are simply related to parton model soft functions and which allow tests of the underlying parton dynamics. In Section IV we study in detail what information can be extracted about the parton densities and fragmentation functions.Conclusions follow in Section V.II.THE INDEPENDENT OBSER V ABLES OF THE REACTIONWe consider the reactionℓ(λ)+N(µ)→H(h)+ℓ′+X(1) of a charged leptonℓwith helicityλ=±1/2on a nucleon N of helicityµ=±1/2producing, semi-inclusively,a spin1/2hyperon H with helicity h=±1/2.The hyperon H is such that its polarization can be determined from its decay distribution.We consider kinematical regions where Z exchange is negligible.The fundamental invariant differential cross section will be written asdσH hλµThe longitudinal or helicity polarization of H,as produced from a given initial state(λµ)is then given byP Hλµ=dσH+λµ−dσH−λµ2(dσH h+µ+dσH h−µ).(7)Because of(5)there will be only four independent cross sections or observables,instead of the original2×2×2=8.We shall take as the four independent cross sections:a)The unpolarized cross sectiondσH≡dσH00=12(dσH+++dσH+−).(8)b)The target-spin dependent cross section difference∆dσH≡dσH++−dσH+−.(9) c)The spin-transfer cross section from a polarized lepton with an unpolarized nucleondσH+−H−+0≡dσH++0−dσH−+0=P H+0dσH,(10)where we have chosen a positive helicity for the lepton and have used,via(5),dσH+0=dσH−0=dσH0+=dσH0−=dσH.(11) Clearly,also via(5)dσH+−H−+0=−dσH+−H−−0.(12)d)The spin-transfer cross section from a polarized nucleon with an unpolarized leptondσH+−H−0+≡dσH+0+−dσH−0+=P H0+dσH.(13)Since these are four linearly independent observables,all others can be written in terms of them.For example it is easy to see thatdσH+−H−++=dσH+−H−+0+dσH+−H−0+(14)anddσH+−H−+−=dσH+−H−+0−dσH+−H−0+.(15)In terms of the hyperon polarization,(14)and(15)implyP H++=1dσH++P H+0+P H0+ (16)andP H+−=1dσH+−P H+0−P H0+ .(17)Note that equations like(16)and(17)are not predictions of the detailed dynamics,but follow from parity invariance of the strong and electromagnetic interactions.Similar relations were given in[1].III.THE DYNAMICAL MODELIn LO pQCD,the general cross section(2)corresponding to the process in(1)is given bydσH hλµdy D H h qλq(z),(18)where the sum is over quarks and antiquarks,qµλq(x)is the parton number density for quarks of helicityλq in a proton of helicityµ,while D H h qλqis the fragmentation function for a quarkq of helicityλq to fragment into hyperon H with helicity h;dˆσλλq /dy is the lepton-quark(or antiquark)differential cross section for an initial state with the lepton having helicityλand the quark(or antiquark)helicityλq.The simple helicity structure of(18)reflects the fact that helicity is conserved for massless quarks inℓq→ℓq.There are two independent partonic cross sectionsdˆσ++dy =4πα2dy =dˆσ−+sxy2(1−y)2,(20)where s is the squared centre of mass energy corresponding to the process in Eq.(1).In order to simplify the expressions needed for theflavour analysis,we renormalize our four independent cross sections(8-10),(13),by dividing out certain common kinematic factors. Thus we work witha′)d˜σH(x,z)≡ 2πα2y2 −1dσH= q e2q q(x)D H q(z),(21)where q(x)and D H q(z)are the usual unpolarized parton density and fragmentationfunctions respectively,q(x)=q++(x)+q+−(x),D H q(z)=D H+q+(z)+D H−q+(z).b′)∆d˜σH(x,z)≡ 4πα2y2 −1∆dσH= q e2q∆q(x)D H q(z),(22) where∆q(x)=q++(x)−q+−(x)is the usual longitudinally polarized parton density. c′)d˜σH+−H−+0(x,z)≡ 2πα2y2 −1dσH+−H−+0= q e2q q(x)∆D H q(z),(23) where∆D H q(z)=D H+q+(z)−D H−q+(z)=D H+q+(z)−D H+q−(z).(24)d′)d˜σH+−H−0+(x,z)≡ 2πα2y2 −1dσH+−H−0+= q e2q∆q(x)∆D H q(z).(25)We see that for eachflavour,for a given hyperon H and for a given target,the four indepen-dent cross sections just correspond to different combinations of the four independent soft functions,q(x),∆q(x),D H q(z),∆D H q(z).It should be noted that the fact that d˜σH,∆d˜σH,d˜σH+−H−+0,d˜σH+−H−0+depend only onx and z(neglecting the known and mild dependence on Q2=xys,due to QCD evolution) is a direct consequence of the parton dynamics and should be tested experimentally.IV.EXTRACTION OF PARTON DENSITIES AND FRAGMENTATIONFUNCTIONSWe assume that the usual unpolarized parton densities u(x),d(x),¯u(x),¯d(x)are reason-ably well known and can be used as input in the following expressions.We consider the production ofΛand¯Λhyperons on both proton and neutron targets and show how one can systematically obtain information about the parton densities s(x),¯s(x),∆s(x),∆¯s(x)and about the fragmentation functions∆DΛu(z),∆DΛd(z),∆DΛs(z).We shall assume good enough control over systematic errors to allow us to combine cross sections for different targets and forΛand¯Λfinal particles.This is a non-trivial experi-mental issue,but well worth the effort,since it then becomes possible to obtain very simple expressions for the parton densities and fragmentation functions under study.A.Unpolarized cross sectionUsing only charge conjugation invariance,DΛq=D¯Λ¯q,(26) and isospin invariance,DΛd=DΛu,(27) we obtain from(21)the well known relations[13]d˜σΛ+¯Λ p−d˜σΛ+¯Λ n=13[u v(x)−d v(x)]DΛ−¯Λu(z),(29)where q v(x)is a valence quark density.Measurements of the cross section differences on the LHS of(28)and(29)thus enable adetermination of DΛ+¯Λu and DΛ−¯Λuand therefore of the individual DΛu and D¯Λu.Next we consider the combinationsd˜σΛ+¯Λ p+d˜σΛ+¯Λ n=59[s(x)+¯s(x)]DΛ+¯Λs(z),(30)d˜σΛ−¯Λ p+d˜σΛ−¯Λ n=59[s(x)−¯s(x)]DΛ−¯Λs(z).(31)Since we now know DΛ±¯Λu,(30)and(31)allow a determination of the productsS1(x,z)≡[s(x)+¯s(x)]DΛ+¯Λs(z)(32) andS2(x,z)≡[s(x)−¯s(x)]DΛ−¯Λs(z).(33) In usual DIS it is the combination(s+¯s)that appears,so if this is taken as reasonably welldetermined we can extract information on DΛ+¯Λs (z)from Eq.(32).Of more interest is thequestion of whether the nucleon possesses intrinsic strange quarks,such that s(x)=¯s(x)[14].Since DΛ−¯Λs (z)is likely to be relatively large,a measurement of(33)should enable oneto say whether(s−¯s)is compatible with zero.For further discussion of the evaluation of (s−¯s)see Ref.[13].B.Cross section for unpolarized lepton and polarized nucleon target Analogously to(28-31)we now have from(22)∆d˜σΛ+¯Λ p−∆d˜σΛ+¯Λ n=13[∆u v(x)−∆d v(x)]DΛ−¯Λu(z),(35)where∆q v is defined as∆q−∆¯q.As stressed in[13],(34)and(28)provide a stringent test for the reliability of the LO treatment.By taking their ratio one obtains in LO∆AΛ+¯Λp−n (x,z,Q2)≡∆d˜σΛ+¯Λ p−∆d˜σΛ+¯Λ n(F p1−F n1)LO(x,Q2),(36)where g1and F1are the usual polarized and unpolarized DIS structure functions,here evaluated in LO.The crucial feature of(36)is that,in principle,the LHS depends on three variables(x,z,Q2),and only in LO should it be independent of z,the so called passive variable[13].It is essential to test this feature in order to have any confidence in the LO treatment.For the experimental situation under discussion in this subsection we can write equations analogous to(30)and(31)via the substitutionsd˜σ→∆d˜σand q(x)→∆q(x).(37) In this case we learn about the products∆S1(x,z)≡[∆s(x)+∆¯s(x)]DΛ+¯Λs(z)(38) and∆S2(x,z)≡[∆s(x)−∆¯s(x)]DΛ−¯Λs(z).(39)Assuming DΛ+¯Λs has been determined as in Section A,(38)would give valuable informationabout(∆s+∆¯s)which is only poorly determined from polarized DIS[11].And(39)could provide an answer to the intriguing question as to whether or not∆s(x)=∆¯s(x),see comments after Eq.(33).In addition the ratios∆S1(x,z)s(x)+¯s(x),(40)∆S2(x,z)s(x)−¯s(x),(41)should be independent of the passive variable z.C.PolarizedΛand¯Λproduction with polarized lepton and unpolarized nucleonWith a polarized lepton beam and unpolarized nucleon target,the difference between cross sections to produceΛ’s or¯Λ’s with helicity±1/2is given by(23).To simplify the notation,let us writed˜σΛ+−Λ−+0≡d˜σ∆Λ+0,etc (42)Then,from(23)we obtain four equations analogous to(28),(29),(30),(31):d˜σ∆Λ+∆¯Λ+0 p−d˜σ∆Λ+∆¯Λ+0 n=13[u v(x)−d v(x)]∆DΛ−¯Λu(z),(44)from which we can determine∆DΛu(z)and∆D¯Λu(z),andd˜σ∆Λ+∆¯Λ+0 p+d˜σ∆Λ+∆¯Λ+0 n=59[s(x)+¯s(x)]∆DΛ+¯Λs(z),(45)d˜σ∆Λ−∆¯Λ+0 p+d˜σ∆Λ−∆¯Λ+0 n=59[s(x)−¯s(x)]∆DΛ−¯Λs(z),(46)yielding information on the productsS3(x,z)≡[s(x)+¯s(x)]∆DΛ+¯Λs(z),(47)S4(x,z)≡[s(x)−¯s(x)]∆DΛ−¯Λs(z).(48)Eq.(47)yields information on∆DΛ+¯Λs (z)and(48)provides a further test of whether s(x)=¯s(x).D.PolarizedΛand¯Λproduction with polarized nucleon and unpolarized lepton Analogous to(43)and(44),we haved˜σ∆Λ+∆¯Λ0+ p−d˜σ∆Λ+∆¯Λ0+ n=13[∆u v(x)−∆d v(x)]∆DΛ−¯Λu(z).(50)The ratio of(49)and(43)provides a further test of the reliability of a LO treatment.One hasd˜σ∆Λ+∆¯Λ0+ p−d˜σ∆Λ+∆¯Λ0+n(F p1−F n1)LO(x,Q2),(51) in LO.The analogues of(45)and(46)are obtained by the substitutiond˜σ∆Λ±∆¯Λ+0→d˜σ∆Λ±∆¯Λ0+and q(x)→∆q(x),(52)and yield information on∆S3(x,z)=[∆s(x)+∆¯s(x)]∆DΛ+¯Λs(z),(53)∆S4(x,z)=[∆s(x)−∆¯s(x)]∆DΛ−¯Λs(z).(54) The ratios∆S3(x,z)(55)s(x)+¯s(x)and∆S4(x,z)(56)s(x)−¯s(x)should be independent of z in LO and should equal the ratios∆S1/S1and∆S2/S2respec-tively,determined in Section B[see(40)and(41)].V.CONCLUSIONSThe study of the angular distribution of theΛ→pπdecay allows a simple and direct measurement of the components of theΛpolarization vector.ForΛ’s produced in the cur-rent fragmentation region in DIS processes,the components of the polarization vector are related to spin properties of the quark inside the nucleon,to spin properties of the quark hadronization,and to spin dynamics of the elementary interactions.All this information, concerning quark distribution functions,quark fragmentation functions and spin properties of elementary dynamics are essentially factorized in LO QCD and separated as depending on three different variables,respectively x,z,y.The Q2-evolution and dependence of distribu-tion and fragmentation functions somewhat mix the three variables,but smoothly,keeping separated the main properties of each of the different aspects of the process.Moreover,such Q2-dependence is perturbatively well known and under control.We have discussed all dif-ferent longitudinal polarization states of spin-1/2baryons,obtainable in the fragmentation of a quark in DIS with longitudinally polarized initial leptons and nucleons.We have shown how one can extract new information,not attainable in unpolarized in-clusive DIS,about parton densities,and new information,not extractable from e+e−→hadrons,about fragmentation functions.In particular one can learn about the poorly known polarized strange quark density∆s(x)+∆¯s(x)and one can get some information relevant to the question as to whether s(x)=¯s(x)and whether∆s(x)=∆¯s(x).The connection between the theoretical quantities and the combinations of measured cross sections is very simple,but the challenge will be an experimental one,namely to have sufficient control over systematic errors so as to permit the combining of different measurements.We hope this will soon be possible.ACKNOWLEDGMENTSWe are very grateful to P.Mulders and the Theory Division of the Physics Department, Vrije Universiteit Amsterdam,where this work was initiated,for the warm hospitality.M.B. is most grateful for support from the EU-TMR Program,Contract No.CT98-0169.U.D. and F.M.are grateful to COFINANZIAMENTO MURST-PRIN for partial support. 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